|
| 2774 | \exists \varepsilon :\ \forall x\left|x-x_0\right|<\varepsilon \Rightarrow f\left(x\right)\le f\left(x_0\right) | |
| 2775 | \exists \varepsilon :\ \forall x\left|x-x_0\right|<\varepsilon \Rightarrow f\left(x\right)>f\left(x_0\right) | |
| 2776 | \exists \varepsilon :\ \forall x\left|x-x_0\right|<\varepsilon \Rightarrow f\left(x\right)\ge f\left(x_0\right) | |
| 2777 | f:\left[a,b\right]\to \mathbb{R} | |
| 2778 | f\left(a\right)f\left(b\right)<0 | |
| 2779 | x_0\in \left[a,b\right] | |
| 2780 | f\left(x_0\right)=0 | |
| 2781 | x_0\in \left[a,b\right] | |
| 2782 | f\left(x_0\right)\neq 0 | |
| 2783 | x_0\in \left[a,b\right] | |
| 2784 | f\left(x_0\right)=0 | |
| 2785 | x_0\in \left[a,b\right] | |
| 2786 | f\left(x_0\right)\neq 0 | |
| 2787 | x_0\in \left[a,b\right] | |
| 2788 | f\left(x_0\right)=0 | |
| 2789 | f:A\to \mathbb{R} | |
| 2790 | A\subseteq \mathbb{R} | |
| 2791 | f | |
| 2792 | A | |
| 2793 | f | |
| 2794 | A | |
| 2795 | A | |
| 2796 | f | |
| 2797 | A | |
| 2798 | A | |
| 2799 | f | |
| 2800 | A | |
| 2801 | A | |
| 2802 | f | |
| 2803 | A | |
| 2804 | f | |
| 2805 | A | |
| 2806 | y=2\left|{\sin x}\right|-2 | |
| 2807 | x=0 | |
| 2808 | x=\frac{\pi }{2} | |
| 2809 | x=k\pi | |
| 2810 | k\in \mathbb{N} | |
| 2811 | x=\frac{\pi }{2}+k\pi | |
| 2812 | k\in \mathbb{N} | |
| 2813 | f\left(x\right)={\sin x} | |
| 2814 | g\left(x\right)={\cos x} | |
| 2815 | x\in \left[0,2\pi \right] | |
| 2816 | f\left(x\right)=e^x | |
| 2817 | g\left(x\right)=-{\arctan x} | |
| 2818 | \mathbb{R} | |
| 2819 | f\left(x\right)>g\left(x\right)\ \forall x\in \mathbb{R} | |
| 2820 | f\left(x\right)\le g\left(x\right)\ \forall x\in \mathbb{R} | |
| 2821 | y | |
| 2822 | f\left(x\right)=e^x | |
| 2823 | g\left(x\right)={\cos x} | |
| 2824 | f\left(x\right)\ge g\left(x\right)\ \forall x | |
| 2825 | f\left(x\right)\le g\left(x\right)\ \forall x | |
| 2826 | f\left(x\right)>g\left(x\right)\ \forall x\ge 0 | |
| 2827 | f\left(x\right)\ge g\left(x\right)\ \forall x\ge 0 | |
| 2828 | f:\mathbb{R}\to \mathbb{R} | |
| 2829 | f:{\mathbb{R}}^2\to \mathbb{R} | |
| 2830 | f:X\to Y | |
| 2831 | x\in X | |
| 2832 | y\in Y | |
| 2833 | x\in X | |
| 2834 | y\in Y | |
| 2835 | y\in Y | |
| 2836 | x\in X | |
| 2837 | y\in Y | |
| 2838 | x\in X | |
| 2839 | y\in Y | |
| 2840 | x\in X | |
| 2841 | f | |
| 2842 | x_0 | |
| 2843 | f | |
| 2844 | x_0 | |
| 2845 | f | |
| 2846 | x_0 | |
| 2847 | f | |
| 2848 | x_0 | |
| 2849 | f^{''} | |
| 2850 | x_0 | |
| 2851 | f^{''} | |
| 2852 | x_0 | |
| 2853 | f:X\to \mathbb{R} | |
| 2854 | X | |
| 2855 | X | |
| 2856 | f\left(X\right)\subseteq \mathbb{R} | |
| 2857 | f\left(X\right)\subseteq \mathbb{R} | |
| 2858 | f\left(X\right)\subseteq \mathbb{R} | |
| 2859 | f:X\to \mathbb{R} | |
| 2860 | X | |
| 2861 | X | |
| 2862 | f\left(X\right)\subseteq \mathbb{R} | |
| 2863 | f\left(X\right)\subseteq \mathbb{R} | |
| 2864 | f:X\to \mathbb{R} | |
| 2865 | f | |
| 2866 | f | |
| 2867 | f | |
| 2868 | f | |
| 2869 | {\lim_{x\to x_0} f\left(x\right)} | |
| 2870 | x\to x^+_0 | |
| 2871 | x\to x^-_0 | |
| 2872 | x\to x^+_0 | |
| 2873 | x\to x^-_0 | |
| 2874 | x\to x^+_0 | |
| 2875 | x\to x^-_0 | |
| 2876 | x\to x^+_0 | |
| 2877 | x\to x^-_0 | |
| 2878 | f\left(x_0\right) | |
| 2879 | x\to x_0 | |
| 2880 | f\left(x\right) | |
| 2881 | x_0 | |
| 2882 | x\to x_0 | |
| 2883 | f\left(x\right) | |
| 2884 | 0 | |
| 2885 | x\to x_0 | |
| 2886 | f\left(x\right) | |
| 2887 | +\infty | |
| 2888 | x\to x_0 | |
| 2889 | f\left(x\right) | |
| 2890 | -\infty | |
| 2891 | x\to x_0 | |
| 2892 | f\left(x\right) | |
| 2893 | 1 | |
| 2894 | x\to x_0 | |
| 2895 | x\to x_0 | |
| 2896 | f\left(x\right) | |
| 2897 | x\_0 | |
| 2898 | x\to x_0 | |
| 2899 | f\left(x\right) | |
| 2900 | 0 | |
| 2901 | x\to x_0 | |
| 2902 | f\left(x\right) | |
| 2903 | \infty | |
| 2904 | x\to x_0 | |
| 2905 | f\left(x\right) | |
| 2906 | 1 | |
| 2907 | x\to x_0 | |
| 2908 | f\left(x\right) | |
| 2909 | f\left(x_0\right) | |
| 2910 | x\to x_0 | |
| 2911 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}} | |
| 2912 | x\neq 0 | |
| 2913 | x_0\neq 0 | |
| 2914 | g\left(x_0\right)\neq 0 | |
| 2915 | g\left(x\right)\neq 0\ \forall x | |
| 2916 | g\left(x\right)\neq 0 | |
| 2917 | x\to x_0 | |
| 2918 | f\left(x\right) | |
| 2919 | g\left(x\right) | |
| 2920 | x\to x_0 | |
| 2921 | f | |
| 2922 | g | |
| 2923 | x\to x_0 | |
| 2924 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}}=0 | |
| 2925 | {\lim_{x\to x_0} \frac{g\left(x\right)}{f\left(x\right)}}=0 | |
| 2926 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}}=l | |
| 2927 | {\lim_{x\to x_0} \frac{g\left(x\right)}{f\left(x\right)}}=l | |
| 2928 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}} | |
| 2929 | g\left(x\right) | |
| 2930 | 0 | |
| 2931 | x\to x_0 | |
| 2932 | f\left(x\right)=o\left(g\left(x\right)\right) | |
| 2933 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}}=0 | |
| 2934 | {\lim_{x\to x_0} \frac{g\left(x\right)}{f\left(x\right)}}=1 | |
| 2935 | {\lim_{x\to x_0} \frac{g\left(x\right)}{f\left(x\right)}}=l | |
| 2936 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}}=+\infty | |
| 2937 | {\lim_{x\to x_0} \frac{f\left(x\right)}{g\left(x\right)}}=-\infty | |
| 2938 | f:\left[a,b\right]\to \mathbb{R} | |
| 2939 | \left[a,b\right] | |
| 2940 | \left(a,b\right) | |
| 2941 | c\in \left[a,b\right]:\frac{f\left(b\right)-f\left(a\right)}{b-a}=f^{'}\left(c\right) | |
| 2942 | c\in \left[a,b\right]:\frac{f\left(b\right)-f\left(a\right)}{b-a}=f\left(c\right) | |
| 2943 | c\in \left[a,b\right]:\frac{f\left(b\right)-f\left(a\right)}{b+a}=f\left(c\right) | |
| 2944 | c\in \left(a,b\right):\frac{f\left(b\right)-f\left(a\right)}{b-a}=f^{'}\left(c\right) | |
| 2945 | c\in \left(a,b\right):\frac{f\left(b\right)-f\left(a\right)}{b+a}=f\left(c\right) | |
| 2946 | x=0 | |
| 2947 | y=\left|x\right| | |
| 2948 | y=x^{\frac{1}{3}} | |
| 2949 | y=\frac{1}{x} | |
| 2950 | y={\ln x} | |
| 2951 | x=0 | |
| 2952 | y={\arctan x} | |
| 2953 | y=\sqrt{x} | |
| 2954 | y=\sqrt[3]{x} | |
| 2955 | y=\frac{1}{x} | |
| 2956 | y=\frac{\left|x\right|}{x-1} | |
| 2957 | x=0 | |
| 2958 | x=1 | |
| 2959 | x=0 | |
| 2960 | x=1 | |
| 2961 | x=1 | |
| 2962 | x=0 | |
| 2963 | x=0 | |
| 2964 | x=1 | |
| 2965 | x=1 | |
| 2966 | x=0 | |
| 2967 | y=\frac{\left|x-2\right|}{x+1} | |
| 2968 | x=2 | |
| 2969 | y=0 | |
| 2970 | y=\frac{1}{3}\left(x-2\right) | |
| 2971 | y=-\frac{1}{3}\left(x-2\right) | |
| 2972 | y=\frac{1}{3}\left(x-2\right) | |
| 2973 | y=-\frac{1}{3}\left(x-2\right) | |
| 2974 | y=\frac{\left|x-3\right|}{x} | |
| 2975 | x=3 | |
| 2976 | f\left(x\right)=e^x | |
| 2977 | g\left(x\right)=x+k | |
| 2978 | k\in \mathbb{R} | |
| 2979 | \left(0,1\right) | |
| 2980 | k=0 | |
| 2981 | k=1 | |
| 2982 | k=e | |
| 2983 | k=\frac{1}{e} | |
| 2984 | k | |
| 2985 | f\left(x\right)=e^x | |
| 2986 | g\left(x\right)={\arctan \left(x+a\right)}+b | |
| 2987 | \left(0,1\right) | |
| 2988 | a=0 | |
| 2989 | b=1 | |
| 2990 | a=1 | |
| 2991 | b=0 | |
| 2992 | a | |
| 2993 | b=-{\arctan a} | |
| 2994 | b | |
| 2995 | a=-{\arctan b} | |
| 2996 | f\left(x\right)={\arctan x} | |
| 2997 | g\left(x\right)=ax^2 | |
| 2998 | a=0 | |
| 2999 | a=1 | |
| 3000 | a={\arctan 1} | |
| 3001 | a={\tan 1} | |
| 3002 | f\left(x\right) | |
| 3003 | g\left(x\right) | |
| 3004 | \left(x_0,y_0\right) | |
| 3005 | f\left(x_0\right)=y_0 | |
| 3006 | g\left(x_0\right)=y_0 | |
| 3007 | f\left(x_0\right)=g\left(x_0\right) | |
| 3008 | f^{'}\left(x_0\right)=g^{'}\left(x_0\right) | |
| 3009 | f\left(x\right)=x^2-kx+1 | |
| 3010 | k\in \mathbb{R} | |
| 3011 | y=x^2-1 | |
| 3012 | y=1-x^2 | |
| 3013 | y=1-\frac{1}{2}x^2 | |
| 3014 | y=\frac{1}{2}x^2 | |
| 3015 | y=-\frac{1}{2}x^2 | |
| 3016 | y=mx+q | |
| 3017 | m,q\in \mathbb{R} | |
| 3018 | y=nx^2 | |
| 3019 | n\in \mathbb{N} | |
| 3020 | t={\ln \left(x+k\right)} | |
| 3021 | k\in \mathbb{R} | |
| 3022 | D=\left\{x:x>0\right\} | |
| 3023 | C=\mathbb{R} | |
| 3024 | D=\mathbb{R} | |
| 3025 | C=\left\{y:y>0\right\} | |
| 3026 | D=\left\{x:x>k\right\} | |
| 3027 | C=\mathbb{R} | |
| 3028 | D=\mathbb{R} | |
| 3029 | C=\left\{y:y>k\right\} | |
| 3030 | D=\left\{x:x>k\right\} | |
| 3031 | C=\left\{y:y>k\right\} | |
| 3032 | f\left(x\right)=1-x^2 | |
| 3033 | g\left(x\right)={\ln \left(x-k\right)} | |
| 3034 | \left(0,1\right) | |
| 3035 | k=0 | |
| 3036 | k=1 | |
| 3037 | k=e | |
| 3038 | k=1-e | |
| 3039 | f:\left(a,b\right)\to \mathbb{R} | |
| 3040 | f | |
| 3041 | x | |
| 3042 | {\lim_{h\to 0} \frac{f\left(x+h\right)-f\left(x\right)}{a-b}} | |
| 3043 | {\lim_{x\to h} \frac{f\left(x+h\right)-f\left(x\right)}{a-b}} | |
| 3044 | {\lim_{h\to 0} \frac{f\left(x+h\right)-f\left(x\right)}{h}} | |
| 3045 | {\lim_{x\to h} \frac{f\left(x+h\right)-f\left(x\right)}{b-a}} | |
| 3046 | {\lim_{x\to h} \frac{f\left(x+h\right)-f\left(x\right)}{h}} | |
| 3047 | f | |
| 3048 | x_0 | |
| 3049 | f | |
| 3050 | x_0 | |
| 3051 | f | |
| 3052 | x_0 | |
| 3053 | f | |
| 3054 | x_0 | |
| 3055 | f | |
| 3056 | x_0 | |
| 3057 | f | |
| 3058 | x_0 | |
| 3059 | f | |
| 3060 | x_0 | |
| 3061 | f | |
| 3062 | x_0 | |
| 3063 | x\to 0 | |
| 3064 | f^{'}\left(x\right) | |
| 3065 | m | |
| 3066 | n | |
| 3067 | m\neq n | |
| 3068 | x_0 | |
| 3069 | f | |
| 3070 | x_0 | |
| 3071 | f | |
| 3072 | x_0 | |
| 3073 | f^{'} | |
| 3074 | x_0 | |
| 3075 | f | |
| 3076 | x_0 | |
| 3077 | f^{'} | |
| 3078 | n- | |
| 3079 | f\left(x\right)={\sin x} | |
| 3080 | n=4k+3 | |
| 3081 | k\in \mathbb{N} | |
| 3082 | f^{\left(n\right)}\left(x\right)={\sin x} | |
| 3083 | f^{\left(n\right)}\left(x\right)={\cos x} | |
| 3084 | f^{\left(n\right)}\left(x\right)=-{\sin x} | |
| 3085 | f^{\left(n\right)}\left(x\right)=-{\cos x} | |
| 3086 | k | |
| 3087 | f\left(x\right)={\sin \left(kx\right)} | |
| 3088 | k\in \mathbb{N} | |
| 3089 | x=0 | |
| 3090 | 0 | |
| 3091 | 1 | |
| 3092 | \frac{\sqrt{2}}{2} | |
| 3093 | k | |
| 3094 | k^{13} | |
| 3095 | f\left(x\right)=e^{kx} | |
| 3096 | k\in \mathbb{R} | |
| 3097 | f^{\left(n\right)}\left(x\right)=ke^x | |
| 3098 | f^{\left(n\right)}\left(x\right)=ke^{kx} | |
| 3099 | f^{\left(n\right)}\left(x\right)=ne^{\left(n-1\right)kx} | |
| 3100 | f^{\left(n\right)}\left(x\right)=k^ne^x | |
| 3101 | f^{\left(n\right)}\left(x\right)=k^ne^{kx} | |
| 3102 | f\left(x\right)=\frac{ax}{x-b} | |
| 3103 | a,b\in \mathbb{R} | |
| 3104 | f^{'}\left(x\right)=\frac{a\left(2x-b\right)}{x-b} | |
| 3105 | f^{'}\left(x\right)=\frac{a\left(2x-b\right)}{{\left(x-b\right)}^2} | |
| 3106 | f^{'}\left(x\right)=-\frac{ab}{x-a} | |
| 3107 | f^{'}\left(x\right)=-\frac{ab}{{\left(x-b\right)}^2} | |
| 3108 | f^{'}\left(x\right)=\frac{ab}{{\left(x-a\right)}^2} | |
| 3109 | f\left(x\right)=xe^x | |
| 3110 | f^{\left(n\right)}\left(x\right)=e^x\left(x+1\right) | |
| 3111 | f^{\left(n\right)}\left(x\right)=nxe^x | |
| 3112 | f^{\left(n\right)}\left(x\right)=\left(x+n\right)e^x | |
| 3113 | f^{\left(n\right)}\left(x\right)=n\left(x+n\right)e^x | |
| 3114 | f^{\left(n\right)}\left(x\right)=e^{x+n} | |
| 3115 | f | |
| 3116 | f\left(a\right)<0 | |
| 3117 | f\left(b\right)>0 | |
| 3118 | \left(a,b\right) | |
| 3119 | \left(a,b\right) | |
| 3120 | \left(a,b\right) | |
| 3121 | \left(a,b\right) | |
| 3122 | f\left(x\right) | |
| 3123 | f\left(0\right)=f\left(2\right)=f\left(4\right)= | |
| 3124 | f\left(x\right) | |
| 3125 | \left(0,2\right) | |
| 3126 | \left(2,4\right) | |
| 3127 | f\left(x\right) | |
| 3128 | \left(0,2\right) | |
| 3129 | \left(2,4\right) | |
| 3130 | f\left(x\right) | |
| 3131 | x=0 | |
| 3132 | x=2 | |
| 3133 | x=4 | |
| 3134 | f\left(x\right) | |
| 3135 | x=1 | |
| 3136 | x=3 | |
| 3137 | f\left(x\right) | |
| 3138 | x=2 | |
| 3139 | f\left(x\right)={\ln \left(x-a\right)} | |
| 3140 | g\left(x\right)=x-b | |
| 3141 | a=b-1 | |
| 3142 | b=a-1 | |
| 3143 | a=b | |
| 3144 | b=-1 | |
| 3145 | a=1 | |
| 3146 | f | |
| 3147 | x_0 | |
| 3148 | x\to x_0 | |
| 3149 | f\left(x_0\right)=f\left(x\right)+f^{'}\left(x_0\right)\left(x-x_0\right)+o\left(x-x_0\right) | |
| 3150 | f\left(x\right)=f\left(x_0\right)+f^{'}\left(x_0\right)\left(x-x_0\right)+o\left(x-x_0\right) | |
| 3151 | f^{'}\left(x_0\right)=f\left(x_0\right)+f^{'}\left(x_0\right)+o\left(x-x_0\right) | |
| 3152 | f^{'}\left(x\right)=f\left(x\right)+f^{'}\left(x_0\right)\left(x-x_0\right)+o\left(x\right) | |
| 3153 | f\left(x\right)=f\left(x_0\right)+f^{'}\left(x_0\right)\left(x-x_0\right)+o\left(x_0\right) | |
| 3154 | f,g:\left(a,b\right)\to \mathbb{R} | |
| 3155 | n | |
| 3156 | x_0\in \left(a,b\right) | |
| 3157 | f | |
| 3158 | g | |
| 3159 | n | |
| 3160 | x_0 | |
| 3161 | f^{\left(n\right)}\left(x\right)=g^{\left(n\right)}\left(x\right) | |
| 3162 | f | |
| 3163 | g | |
| 3164 | n | |
| 3165 | x_0 | |
| 3166 | f^{\left(n\right)}\left(x\right)=g^{\left(n\right)}\left({x}_0\right) | |
| 3167 | f | |
| 3168 | g | |
| 3169 | n | |
| 3170 | x_0 | |
| 3171 | f^{\left(i\right)}\left(x\right)=g^{\left(i\right)}\left(x_0\right)\ \forall i=0,\dots ,n | |
| 3172 | f | |
| 3173 | g | |
| 3174 | n | |
| 3175 | x_0 | |
| 3176 | f^{\left(i\right)}\left(x_0\right)=g^{\left(i\right)}\left(x_0\right)\ \forall i=0,\dots ,n | |
| 3177 | f | |
| 3178 | g | |
| 3179 | n | |
| 3180 | x_0 | |
| 3181 | f^{\left(i\right)}\left(x_0\right)=g^{\left(i\right)}\left(x_0\right)\ \forall i=0,\dots ,n | |
| 3182 | P\left(x\right)=f\left(x_0\right)+f^{'}\left(x_0\right)\left(x-x_0\right)+o\left(x-x_0\right) | |
| 3183 | x\to x_0 | |
| 3184 | f\left(x\right) | |
| 3185 | f\left(x\right) | |
| 3186 | f\left(x\right) | |
| 3187 | f\left(x\right) | |
| 3188 | f\left(x\right)\in C^2\left(\mathbb{R}\right) | |
| 3189 | x_0 | |
| 3190 | f^{'}\left(x_0\right)=0 | |
| 3191 | f^{''}\left(x_0\right)\neq 0 | |
| 3192 | x_0 | |
| 3193 | x_0 | |
| 3194 | f^{\left(n\right)}\left(x_0\right)<0 | |
| 3195 | x_0 | |
| 3196 | f^{''}\left(x_0\right)<0 | |
| 3197 | x_0 | |
| 3198 | x_0 | |
| 3199 | f\left(x\right)\in C^{\infty }\left(\mathbb{R}\right) | |
| 3200 | \ \forall x\in \mathbb{R} | |
| 3201 | \ \forall x\in \mathbb{R} | |
| 3202 | \ \forall x\in \mathbb{R} | |
| 3203 | \ \forall x\in \mathbb{R} | |
| 3204 | f\left(x\right)\in C^{\infty }\left(\mathbb{R}\right) | |
| 3205 | x_0 | |
| 3206 | 8 | |
| 3207 | f\left(x\right) | |
| 3208 | x_0 | |
| 3209 | f^{\left(9\right)}\left(x_0\right)=0 | |
| 3210 | x_0 | |
| 3211 | f | |
| 3212 | f^{\left(9\right)}\left(x_0\right)>0 | |
| 3213 | x_0 | |
| 3214 | f | |
| 3215 | f^{\left(9\right)}\left(x_0\right)<0 | |
| 3216 | x_0 | |
| 3217 | f | |
| 3218 | f^{\left(9\right)}\left(x_0\right)\neq 0 | |
| 3219 | x_0 | |
| 3220 | f | |
| 3221 | {\ln \left(1+x\right)} | |
| 3222 | x-x^2+x^3+o\left(x^3\right) | |
| 3223 | x-\frac{1}{2}x^2+\frac{1}{3}x^3+o\left(x^3\right) | |
| 3224 | x-\frac{1}{2!}x^2+\frac{1}{3!}x^3+o\left(x^3\right) | |
| 3225 | x+\frac{1}{2!}x^2-\frac{1}{3!}x^3+o\left(x^3\right) | |
| 3226 | 1+x-\frac{1}{2!}x^2+\frac{1}{3!}x^3+o\left(x^3\right) | |
| 3227 | {\cos x} | |
| 3228 | 1-\frac{1}{2}x^2+\frac{1}{4}x^4+o\left(x^4\right) | |
| 3229 | x-\frac{1}{3!}x^3+o\left(x^4\right) | |
| 3230 | 1-\frac{1}{2!}x^2+\frac{1}{4!}x^4+o\left(x^4\right) | |
| 3231 | 1-\frac{1}{2!}x^2+\frac{1}{4!}x^4 | |
| 3232 | 1-\frac{1}{2!}x^2+o\left(x^4\right) | |
| 3233 | f\left(x\right)={\sin x}-{\cosh x} | |
| 3234 | f | |
| 3235 | y | |
| 3236 | f | |
| 3237 | y | |
| 3238 | f | |
| 3239 | f | |
| 3240 | f | |
| 3241 | \frac{2}{1+e^x} | |
| 3242 | 1+x+x^3+o\left(x^3\right) | |
| 3243 | 1-x+x^3+o\left(x^3\right) | |
| 3244 | 1+\frac{x}{2}+\frac{x^3}{24}+o\left(x^3\right) | |
| 3245 | 1-\frac{x}{2}+\frac{x^3}{24}+o\left(x^3\right) | |
| 3246 | 1-\frac{x}{2}+\frac{x^3}{24}-\frac{x^5}{240}+o\left(x^5\right) | |
| 3247 | f\left(x\right)={\arctan \sqrt{\frac{1-{\cos x}}{1+{\cos x}}}} | |
| 3248 | x=\frac{\pi }{2}+2k\pi | |
| 3249 | f\left(x\right)=k{\left(x-a\right)}^3 | |
| 3250 | +\infty | |
| 3251 | x\to +\infty | |
| 3252 | -\infty | |
| 3253 | x\to +\infty | |
| 3254 | k<0 | |
| 3255 | -\infty | |
| 3256 | x\to -\infty | |
| 3257 | k<0 | |
| 3258 | +\infty | |
| 3259 | x\to +\infty | |
| 3260 | a<0 | |
| 3261 | +\infty | |
| 3262 | x\to -\infty | |
| 3263 | a>0 | |
| 3264 | f\left(x\right)=\left(x-a\right)\left(x-b\right)\left(x-c\right) | |
| 3265 | a,b,c\in \mathbb{R} | |
| 3266 | a\le b\le c | |
| 3267 | 3 | |
| 3268 | 3 | |
| 3269 | f\left(x\right)=k{\cos \left(kx\right)} | |
| 3270 | k\in \mathbb{R} | |
| 3271 | k | |
| 3272 | k | |
| 3273 | k | |
| 3274 | k | |
| 3275 | f\left(x\right)=e^{-x{\sin x}} | |
| 3276 | g\left(x\right)=-x{\sin \left(kx\right)} | |
| 3277 | g\left(x\right)=-x{\sin \left(kx\right)} | |
| 3278 | g\left(x\right)=x{\sin \left(kx\right)} | |
| 3279 | g\left(x\right)=x{\sin \left(kx\right)} | |
| 3280 | f:\left[a,b\right]\to \mathbb{R} | |
| 3281 | f:\left[a,b\right]\to \mathbb{R} | |
| 3282 | f\left(x\right)=\frac{1}{\sqrt{x}}-2e^x+3 | |
| 3283 | \int{f\left(x\right)dx} | |
| 3284 | \sqrt{x}-e^x + k | |
| 3285 | 2\left(\sqrt{x}-e^x\right) + k | |
| 3286 | 2\left(\sqrt{x}-e^x\right)+3 + k | |
| 3287 | 2\left(\sqrt{x}-e^x\right)+3x + k | |
| 3288 | 2\left(\sqrt{x}-e^x+3x\right) + k | |
| 3289 | f\left(x\right)={\ln x} | |
| 3290 | \int{f\left(x\right)dx} | |
| 3291 | {\ln x}+k | |
| 3292 | {\ln x}-1+k | |
| 3293 | {\ln x}+1+k | |
| 3294 | x\left({\ln x}-1\right)+k | |
| 3295 | x\left({\ln x}+1\right)+k | |
| 3296 | f | |
| 3297 | g | |
| 3298 | f\le g | |
| 3299 | \int{f}>\int{g} | |
| 3300 | \int{f}\ge \int{g} | |
| 3301 | \int{f}<\int{g} | |
| 3302 | \int{f}\le \int{g} | |
| 3303 | \int{f}=\int{g} | |
| 3304 | f\left(x\right) | |
| 3305 | \left[a,b\right] | |
| 3306 | M={sup \left|f\left(x\right)\right|} | |
| 3307 | x\in \left[a,b\right] | |
| 3308 | \left|\int^b_a{f\left(x\right)dx}\right|=M\left(b-a\right) | |
| 3309 | \left|\int^b_a{f\left(x\right)dx}\right|\le M\left(b-a\right) | |
| 3310 | \left|\int^b_a{f\left(x\right)dx}\right|=M\left(a-b\right) | |
| 3311 | \int^b_a{f\left(x\right)dx}\le M\left(a-b\right) | |
| 3312 | \int^b_a{f\left(x\right)dx}=M\left(b-a\right) | |
| 3313 | \int{f}=\int{\left|f\right|} | |
| 3314 | \int{\left|f\right|}\le \int{f} | |
| 3315 | \left|\int{f}\right|\le \int{\left|f\right|} | |
| 3316 | \left|\int{f}\right| = \int{f} | |
| 3317 | \left|\int{f}\right|=\int{\left|f\right|} | |
| 3318 | f\left(x\right) | |
| 3319 | \left[a,b\right] | |
| 3320 | t\in \left[a,b\right] | |
| 3321 | \int^b_a{f\left(x\right)dx}=t\left(b-a\right) | |
| 3322 | \int^b_a{f\left(x\right)dx}=t\left(a-b\right) | |
| 3323 | \int^b_a{f\left(x\right)dx}=f\left(t\right)\left(b-a\right) | |
| 3324 | \int^b_a{f\left(x\right)dx}=f\left(t\right)\frac{1}{\left(a-b\right)} | |
| 3325 | \int^b_a{f\left(x\right)dx}=t\left(b-a\right) | |
| 3326 | f\left(x\right) | |
| 3327 | \left[a,b\right] | |
| 3328 | f | |
| 3329 | \left(b-a\right)\int^b_a{f\left(x\right)dx} | |
| 3330 | \frac{1}{b-a}\int^b_a{f\left(x\right)dx} | |
| 3331 | \left(a-b\right)\int^b_a{f\left(x\right)dx} | |
| 3332 | \frac{1}{a-b}\int^b_a{f\left(x\right)dx} | |
| 3333 | f\left(x\right) | |
| 3334 | a | |
| 3335 | b | |
| 3336 | c | |
| 3337 | A=\int^b_a{f\left(x\right)dx} | |
| 3338 | B=\int^b_c{f\left(x\right)dx} | |
| 3339 | C=\int^c_a{f\left(x\right)dx} | |
| 3340 | A=B+C | |
| 3341 | B=A-C | |
| 3342 | C=A-B | |
| 3343 | f\left(x\right)\in C^0\left[a,b\right] | |
| 3344 | c\in \left[a,b\right] | |
| 3345 | F\left(x\right)=\int^x_c{f\left(t\right)dt} | |
| 3346 | F\in C^0\left[a,b\right] | |
| 3347 | f^{'}\left(x\right)=f\left(x\right)\ \forall x\in \left[a,b\right] | |
| 3348 | F\in C^1\left[a,b\right] | |
| 3349 | f^{'}\left(x\right)=f\left(x\right)\ \forall x\in \left[a,b\right] | |
| 3350 | F\in C^0\left[a,b\right] | |
| 3351 | F\left(x\right)=f^{'}\left(x\right)\ \forall x\in \left(a,b\right) | |
| 3352 | F\in C^1\left(a,b\right) | |
| 3353 | F\left(x\right)=f^{'}\left(x\right)\ \forall x\in \left(a,b\right) | |
| 3354 | F\in C^2\left(a,b\right) | |
| 3355 | f^{'}\left(x\right)=f\left(x\right)\ \forall x\in \left(a,b\right) | |
| 3356 | \int{f\left(x\right)dx} | |
| 3357 | f | |
| 3358 | f | |
| 3359 | f | |
| 3360 | f | |
| 3361 | f | |
| 3362 | f\left(x\right)={{\sin}^{2} x} | |
| 3363 | \int f\left(x\right)dx | |
| 3364 | {{\cos}^{2} x}+k | |
| 3365 | \frac{1}{2}{\cos 2x}+k | |
| 3366 | \frac{1}{2}\left(x-\cos 2x\right)+k | |
| 3367 | \frac{1}{2}\left(x-\sin x\cos x\right)+k | |
| 3368 | \frac{1}{2}\left(x-\sin 2x\cos 2x\right)+k | |
| 3369 | a,b,n\in \mathbb{R} | |
| 3370 | \int{na^b}da | |
| 3371 | a^b+k | |
| 3372 | \frac{na^b}{{\ln a}}+k | |
| 3373 | \frac{a^b}{{\ln a}}+k | |
| 3374 | \frac{n}{b+1}a^b+k | |
| 3375 | \frac{n}{b+1}a^{b+1}+k | |
| 3376 | a,b,c\in \mathbb{R} | |
| 3377 | \int{a^b{\cos c}}dc | |
| 3378 | \frac{a^{b+1}}{b+1}\cos c | |
| 3379 | \frac{a^{b+1}}{b+1}\sin c | |
| 3380 | a^b \sin c | |
| 3381 | \frac{a^b}{\ln a} \cos c | |
| 3382 | \frac{a^{b+1}}{{\ln a}}{\sin c} | |
| 3383 | f\left(x\right)={{\tan}^{2} x} | |
| 3384 | \int{f\left(x\right)dx} | |
| 3385 | {\tan x}+k | |
| 3386 | {{\tan}^{2} x}+k | |
| 3387 | {\tan x}-x+k | |
| 3388 | {\tan x}+x+k | |
| 3389 | {\tan x}+x^2+k | |
| 3390 | f\left(x\right)=\frac{\sqrt{1+x}}{\sqrt{1-x}}+\frac{\sqrt{1-x}}{\sqrt{1+x}} | |
| 3391 | \int{f\left(x\right)dx} | |
| 3392 | {\arcsin x}+k | |
| 3393 | {\arccos 2x}+k | |
| 3394 | 2{\arccos 2x}+k | |
| 3395 | 2{\arcsin x}+k | |
| 3396 | {{\arcsin}^{2} 2x}+k | |
| 3397 | f\left(x\right)=\frac{3}{x{\ln x}} | |
| 3398 | \int{f\left(x\right)dx} | |
| 3399 | {\ln {\ln x}}+k | |
| 3400 | {\ln \left|{\ln x}\right|}+k | |
| 3401 | {\ln {{\ln}^{2} x}}+k | |
| 3402 | 3\ln {\ln x}+k | |
| 3403 | 3\ln \left|{\ln x}\right|+k | |
| 3404 | f\left(x\right)=\frac{e^{\frac{1}{x}}}{x^2} | |
| 3405 | \int{f\left(x\right)dx} | |
| 3406 | e^{2x}+k | |
| 3407 | e^{\frac{1}{x}}+k | |
| 3408 | -e^{\frac{1}{x}}+k | |
| 3409 | e^{\frac{1}{x^2}}+k | |
| 3410 | -2e^{\frac{1}{x}}+k | |
| 3411 | f\left(x\right)=\frac{x}{x-7} | |
| 3412 | \int{f\left(x\right)dx} | |
| 3413 | x+{\ln \left|x+7\right|}+k | |
| 3414 | x-7 \ln \left|x+7\right| +k | |
| 3415 | x+7 \ln \left|x-7\right| +k | |
| 3416 | 7\left(x-{\ln \left|x+7\right|}\right)+k | |
| 3417 | 7\left(x+{\ln \left|x-7\right|}\right)+k | |
| 3418 | f\left(x\right)=\frac{7}{{\sin x}} | |
| 3419 | \int{f\left(x\right)dx} | |
| 3420 | {\tan {\ln \left|\frac{x}{2}\right|}}+k | |
| 3421 | {\ln \left|{\cos x}\right|}+k | |
| 3422 | {\ln \left|7{\cos x}\right|}+k | |
| 3423 | 7{\ln \left|{\tan \frac{x}{2}}\right|}+k | |
| 3424 | {\tan \left(7{\ln \left|\frac{x}{2}\right|}\right)}+k | |
| 3425 | f\left(x\right)=\frac{x^4+x^3+6}{x^2+x} | |
| 3426 | \int{f\left(x\right)dx} | |
| 3427 | x^3+3{\ln \left|\frac{x}{x+1}\right|}+k | |
| 3428 | \frac{1}{3}\left(x^3+6{\ln \left|\frac{x}{x+1}\right|}\right)+k | |
| 3429 | \frac{1}{3}\left(x^3+18{\ln \left|\frac{x}{x+1}\right|}\right)+k | |
| 3430 | 3\left(x^3+\frac{1}{3}{\ln \left|\frac{x}{x+1}\right|}\right)+k | |
| 3431 | 3\left(\frac{1}{3}x^3+18{\ln \left|\frac{x}{x+1}\right|}\right)+k | |
| 3432 | f\left(x\right)=\frac{1}{1+e^x} | |
| 3433 | \int{f\left(x\right)dx} | |
| 3434 | x+{\ln \left(e^x+1\right)}+k | |
| 3435 | {\ln \left(e^x+1\right)}+k | |
| 3436 | x-{\ln \left(e^x+1\right)}+k | |
| 3437 | -{\ln \left(e^x+1\right)}+k | |
| 3438 | {\ln \left(e^x+1\right)}-x+k | |
| 3439 | f\left(x\right)=\frac{{\cos {\ln x}}}{x} | |
| 3440 | \left(e^{\frac{\pi }{2}},1\right) | |
| 3441 | {\cos {\ln \left|x\right|}}+e | |
| 3442 | {\sin {\ln \left|x\right|}} | |
| 3443 | {\ln \left|{\cos x}\right|}+\pi /2 | |
| 3444 | {\cos {\ln \left|x\right|}} | |
| 3445 | {\ln \left|{\sin x}\right|}+1 | |
| 3446 | f\left(x\right)=\frac{k}{x^2+4} | |
| 3447 | k\in \mathbb{R} | |
| 3448 | g\left(x\right)=2{arctan f\left(x\right)}+k | |
| 3449 | \int{f\left(x\right)dx}=g\left(x\right) | |
| 3450 | k=2 | |
| 3451 | f\left(x\right)=2x | |
| 3452 | k=\frac{1}{2} | |
| 3453 | f\left(x\right)=x | |
| 3454 | k=-4 | |
| 3455 | f\left(x\right)=-\frac{x}{2} | |
| 3456 | k=4 | |
| 3457 | f\left(x\right)=\frac{x}{2} | |
| 3458 | k=\frac{1}{4} | |
| 3459 | f\left(x\right)=\frac{x}{2} | |
| 3460 | f\left(x\right)=\frac{kx}{e^x} | |
| 3461 | k\in \mathbb{R} | |
| 3462 | g\left(x\right)=-\frac{k\left(x+1\right)}{e^x}+k | |
| 3463 | \int{f\left(x\right)dx}=g\left(x\right) | |
| 3464 | k=1 | |
| 3465 | k=-1 | |
| 3466 | k=e | |
| 3467 | k | |
| 3468 | k | |
| 3469 | f\left(x\right)=\frac{{\sin x}}{1-2{\cos x}} | |
| 3470 | \int{f\left(x\right)dx} | |
| 3471 | 2\left({\ln \left|f\left(x\right){\cos x}\right|}\right)+k | |
| 3472 | \frac{1}{2}\left({\ln \left|\frac{{\sin x}}{f\left(x\right)}\right|}\right)+k | |
| 3473 | \frac{1}{2}\left({\ln \left|f\left(x\right)\right|}\right)+k | |
| 3474 | 2\left({\ln \left|2f\left(x\right){\cos x}\right|}\right)+k | |
| 3475 | 2\left({\ln \left|\frac{1}{f\left(x\right)}\right|}\right)+k | |
| 3476 | f\left(x\right)=\frac{x+2}{x-1} | |
| 3477 | \left[2,e+1\right] | |
| 3478 | \frac{1+e}{e-1} | |
| 3479 | \frac{2+e}{e-2} | |
| 3480 | \frac{1+e}{2-e} | |
| 3481 | \frac{2+e}{e-1} | |
| 3482 | \frac{2+e}{1-e} | |
| 3483 | f\left(x\right)=\frac{x}{1+x^2} | |
| 3484 | \left[0,2\right] | |
| 3485 | \frac{{\ln 5}}{2} | |
| 3486 | \frac{{\ln 5}}{4} | |
| 3487 | \frac{{\ln 5}}{8} | |
| 3488 | \frac{{\ln 5}}{2} | |
| 3489 | \frac{{\ln 5}}{5} | |
| 3490 | f\left(x\right)=\frac{k}{\sqrt{x}} | |
| 3491 | k\in \mathbb{R} | |
| 3492 | \frac{12}{5} | |
| 3493 | \left[4,9\right] | |
| 3494 | k=1 | |
| 3495 | k=2 | |
| 3496 | k=3 | |
| 3497 | k=6 | |
| 3498 | k=12 | |
| 3499 | \frac{1}{2}{\sin 4x} | |
| 3500 | \left\{a_n\right\} | |
| 3501 | a_n | |
| 3502 | \left\{s_n\right\} | |
| 3503 | s_n=\sum^{\infty }_{n=0}{{\left(a_n\right)}^2} | |
| 3504 | s_n=\sum^{\infty }_{n=0}{a_n} | |
| 3505 | s_n=\prod^{\infty }_{n=0}{\frac{1}{a_n}} | |
| 3506 | s_n=\sum^{\infty }_{n=0}{\sqrt{a_n}} | |
| 3507 | s_n={\lim_{n\to +\infty } a_n} | |
| 3508 | \left\{a_n\right\} | |
| 3509 | s_n = \sum_{k=1}^n a_k | |
| 3510 | a_n | |
| 3511 | a_n | |
| 3512 | a_n | |
| 3513 | a_n | |
| 3514 | n- | |
| 3515 | s_n | |
| 3516 | a_n | |
| 3517 | \left\{a_n\right\} | |
| 3518 | \left\{a_n\right\} | |
| 3519 | \left\{s_n\right\} | |
| 3520 | \left\{s_n\right\} | |
| 3521 | \left\{s_n\right\} | |
| 3522 | \left\{a_n\right\} | |
| 3523 | \left\{s_n\right\} | |
| 3524 | a_n | |
| 3525 | \left\{s_n\right\} | |
| 3526 | \left\{a_n\right\} | |
| 3527 | \left\{s_n\right\} | |
| 3528 | \left\{a_n\right\} | |
| 3529 | \left\{s_n\right\} | |
| 3530 | \left\{a_n\right\} | |
| 3531 | \left\{s_n\right\} | |
| 3532 | \left\{s_n\right\} | |
| 3533 | \left\{s_n\right\} | |
| 3534 | \left\{s_n\right\} | |
| 3535 | \left\{s_n\right\} | |
| 3536 | \left\{s_n\right\} | |
| 3537 | \sum^{\infty }_{n=0}{a_n} | |
| 3538 | \sum^{\infty }_{n=0}{{\left(a_n\right)}^2} | |
| 3539 | \sum^{\infty }_{n=0}{\frac{1}{a_n}} | |
| 3540 | \sum^{\infty }_{n=0}{\left(a_n-a_{n+1}\right)} | |
| 3541 | \sum^{\infty }_{n=0}{\left(a_n-a_{n+2}\right)} | |
| 3542 | \sum^{\infty }_{n=0}{a_n} | |
| 3543 | \varepsilon >0 | |
| 3544 | N | |
| 3545 | \ \forall i\ge 0 | |
| 3546 | \ \forall j\ge n | |
| 3547 | \left|a_i+a_{i+1}+...+a_{i+j}\right|<\varepsilon | |
| 3548 | \varepsilon >0 | |
| 3549 | N | |
| 3550 | \ \forall i\ge 0 | |
| 3551 | \ \forall j\ge n | |
| 3552 | \left|a_i+a_{i+1}+...+a_{i+j}\right|>\varepsilon | |
| 3553 | \varepsilon >0 | |
| 3554 | N | |
| 3555 | \ \forall i\ge N | |
| 3556 | \ \forall j\ge 0 | |
| 3557 | \left|a_i+a_{i+1}+...+a_{i+j}\right|<\varepsilon | |
| 3558 | \varepsilon >0 | |
| 3559 | N | |
| 3560 | \ \forall i\ge N | |
| 3561 | \ \forall j\ge 0 | |
| 3562 | \left|a_i+a_{i+1}+...+a_{i+j}\right|>\varepsilon | |
| 3563 | \sum^{\infty }_{n=1}{n} | |
| 3564 | \sum^{\infty }_{n=1}{n^2} | |
| 3565 | \sum^{\infty }_{n=1}{\frac{1}{n}} | |
| 3566 | \sum^{\infty }_{n=1}{\frac{1}{n^2}} | |
| 3567 | \sum^{\infty }_{n=1}{\frac{1}{\sqrt{n}}} | |
| 3568 | \sum^{\infty }_{n=0}{a_n} | |
| 3569 | \sum^{\infty }_{n=0}{b_n} | |
| 3570 | a_n\sim b_n | |
| 3571 | b_n | |
| 3572 | a_n\sim b_n | |
| 3573 | b_n | |
| 3574 | a_n | |
| 3575 | a_n\sim b_n | |
| 3576 | b_n | |
| 3577 | a_n | |
| 3578 | a_n\sim b_n | |
| 3579 | b_n | |
| 3580 | a_n | |
| 3581 | a_n\sim b_n | |
| 3582 | \sum^{\infty }_{n=0}{a_n} | |
| 3583 | {\lim_{n\to +\infty } \frac{a_{n+1}}{a_n}}=l | |
| 3584 | l<1 | |
| 3585 | l\ge 1 | |
| 3586 | l\le 1 | |
| 3587 | l>1 | |
| 3588 | l\le 1 | |
| 3589 | \sum^{\infty }_{n=0}{a_n} | |
| 3590 | \sum^{\infty }_{n=0}{\left|a_n\right|} | |
| 3591 | \sum^{\infty }_{n=0}{\left|a_n\right|} | |
| 3592 | \sum^{\infty }_{n=0}{a_n} | |
| 3593 | \sum^{\infty }_{n=0}{a_n} | |
| 3594 | \sum^{\infty }_{n=0}{\left|a_n\right|} | |
| 3595 | \sum^{\infty }_{n=0}{\left|a_n\right|} | |
| 3596 | \sum^{\infty }_{n=0}{a_n} | |
| 3597 | \sum^{\infty }_{n=0}{a_n} | |
| 3598 | \sum^{\infty }_{n=0}{\left|a_n\right|} | |
| 3599 | \sum^{\infty }_{n=0}{\left|a_n\right|} | |
| 3600 | \sum^{\infty }_{n=0}{\frac{1}{\left|a_n\right|}} | |
| 3601 | \sum^{\infty }_{n=0}{\frac{1}{\left|a_n\right|}} | |
| 3602 | \sum^{\infty }_{n=1}{\frac{1}{n^k}} | |
| 3603 | k=1 | |
| 3604 | k>1 | |
| 3605 | k=0 | |
| 3606 | k>0 | |
| 3607 | k>=1 | |
| 3608 | \sum^{\infty }_{n=1}{\frac{n+e^{-n}}{n^2-\ln\left(n\right)}} | |
| 3609 | \sum^{\infty }_{n=1}{\frac{2^n}{3^n-n}} | |
| 3610 | \sum^{\infty }_{n=1}{\frac{n!}{n^n}} | |
| 3611 | \sum^{\infty }_{n=1}{\frac{\left(2n\right)!}{{\left(n!\right)}^2}} | |
| 3612 | \sum^{\infty }_{n=1}{\frac{1+{\cos n}}{n^2}} | |
| 3613 | \sum^{\infty }_{n=1}{\frac{k^n}{n^2}} | |
| 3614 | k>1 | |
| 3615 | k<1 | |
| 3616 | k\le 1 | |
| 3617 | k\ge 1 | |
| 3618 | k=1 | |
| 3619 | \sum^{\infty }_{n=1}{{\left(\ln\left(\frac{4n+5}{3n-2}\right)\right)}^n} | |
| 3620 | \sum^{\infty }_{n=1}{\frac{{\cos n}}{n^2-2n-3}} | |
| 3621 | A=\sum^{\infty }_{n=1}{\frac{4}{n+{\ln n}}} | |
| 3622 | B=\sum^{\infty }_{n=1}{\frac{e^n}{{\sinh n}}} | |
| 3623 | C=\sum^{\infty }_{n=1}{\frac{e^n}{2^n+5^n}} | |
| 3624 | A | |
| 3625 | C | |
| 3626 | A | |
| 3627 | B | |
| 3628 | B | |
| 3629 | A | |
| 3630 | A | |
| 3631 | B | |
| 3632 | C | |
| 3633 | B | |
| 3634 | A | |
| 3635 | C | |
| 3636 | A=\sum^{\infty }_{n=1}{\frac{1}{n^5{\ln n}}} | |
| 3637 | B=\sum^{\infty }_{n=1}{\frac{1}{{\ln \left(n+1\right)}}} | |
| 3638 | C=\sum^{\infty }_{n=1}{\frac{n}{n^2+1}} | |
| 3639 | A | |
| 3640 | B | |
| 3641 | C | |
| 3642 | C | |
| 3643 | B | |
| 3644 | B | |
| 3645 | C | |
| 3646 | A | |
| 3647 | B | |
| 3648 | C | |
| 3649 | B | |
| 3650 | A | |
| 3651 | C | |
| 3652 | F\left(x\right)=\int^x_a{\frac{2{\sin t}}{1+t}dt} | |
| 3653 | \left(-\infty ,-1\right]\cup \left[-1,+\infty \right) | |
| 3654 | \left(-\infty ,-1\right)\cup \left(-1,+\infty \right) | |
| 3655 | \left(-\infty ,-1\right] | |
| 3656 | \left(-1,+\infty \right) | |
| 3657 | \left(-\infty ,-1\right) | |
| 3658 | \int^{+\infty }_0{xe^{-x}}dx | |
| 3659 | e | |
| 3660 | 2e | |
| 3661 | \frac{2}{e} | |
| 3662 | 1 | |
| 3663 | +\infty | |
| 3664 | {\lim_{x\to +\infty } \frac{1}{x^2}\int^x_1{\left(t+\frac{1}{t}\right)dt}} | |
| 3665 | 0 | |
| 3666 | 1 | |
| 3667 | 2 | |
| 3668 | \frac{1}{2} | |
| 3669 | +\infty | |
| 3670 | f | |
| 3671 | \mathbb{R} | |
| 3672 | F\left(x\right)=\int^x_0{f\left(t\right)dt} | |
| 3673 | {\lim_{x\to +\infty } F\left(x\right)} | |
| 3674 | {\lim_{x\to +\infty } F\left(x\right)}=+\infty | |
| 3675 | {\lim_{x\to +\infty } F\left(x\right)}=0 | |
| 3676 | F\left(-1\right)=0 | |
| 3677 | F | |
| 3678 | \mathbb{R} | |
| 3679 | \int^{+\infty }_{-\infty }{\frac{\left|x\right|}{9x^2+1}dx} | |
| 3680 | 0 | |
| 3681 | 1 | |
| 3682 | \pi | |
| 3683 | e | |
| 3684 | +\infty | |
| 3685 | \int^{+\infty }_{-\infty }{\frac{1}{x^2+1}dx} | |
| 3686 | \pi | |
| 3687 | \frac{\pi }{2} | |
| 3688 | \frac{\pi }{4} | |
| 3689 | 0 | |
| 3690 | +\infty | |
| 3691 | f:\mathbb{R}\to \mathbb{R} | |
| 3692 | f\left(x\right)=-f\left(-x\right) | |
| 3693 | \int^1_0{f\left(x\right)dx}=0 | |
| 3694 | \int^1_{-1}{f\left(x\right)dx}=0 | |
| 3695 | \int^1_{-1}{f^2\left(x\right)dx}=0 | |
| 3696 | \int^1_{-1}{f\left(x\right)dx}=2\int^1_{-1}{f\left(x\right)dx} | |
| 3697 | \int^1_{-1}{f\left(x\right)dx}=2\int^1_0{f^2\left(x\right)}dx | |
| 3698 | f:\mathbb{R}\to \mathbb{R} | |
| 3699 | \int^3_{-1}{f\left(x\right)dx}=8 | |
| 3700 | x_0\in \left[-1,3\right] | |
| 3701 | f\left(x_0\right)=1 | |
| 3702 | f\left(x_0\right)=2 | |
| 3703 | f\left(x_0\right)=3 | |
| 3704 | f\left(x_0\right)=\frac{1}{2} | |
| 3705 | f\left(x_0\right)=\frac{1}{3} | |
| 3706 | z | |
| 3707 | z+\overline{z}=0 | |
| 3708 | z | |
| 3709 | \left|z\right|=\left|z-1\right| | |
| 3710 | z | |
| 3711 | \left|z\right|-2<0 | |
| 3712 | z | |
| 3713 | \left|z\right|-2\ge 0 | |
| 3714 | {\lim_{x\to +\infty } \frac{2x+5{\ln x}}{4x+3{\ln x}}} | |
| 3715 | 0 | |
| 3716 | 1 | |
| 3717 | 2 | |
| 3718 | \frac{1}{2} | |
| 3719 | +\infty | |
| 3720 | {\ln x}=4-x^2 | |
| 3721 | 0 | |
| 3722 | 1 | |
| 3723 | 2 | |
| 3724 | 3 | |
| 3725 | {\arctan x}=2-e^x | |
| 3726 | 0 | |
| 3727 | 1 | |
| 3728 | 2 | |
| 3729 | 3 | |
| 3730 | {\tan x}={\cos x} | |
| 3731 | 0 | |
| 3732 | 1 | |
| 3733 | 2 | |
| 3734 | 3 | |
| 3735 | k | |
| 3736 | {\ln x}=kx | |
| 3737 | 0 |
| 3738 | 0 |
| 3739 | 0 |
| 3740 | 0 |
| 3741 | 0 |
| 3742 | f\left(x\right)=x^3-5x^2+8x-4 | |
| 3743 | x | |
| 3744 | f:\mathbb{R}\to \mathbb{R} | |
| 3745 | x=0 | |
| 3746 | x=2 | |
| 3747 | x=4 | |
| 3748 | f^{'} | |
| 3749 | f | |
| 3750 | f^{'} | |
| 3751 | f | |
| 3752 | f^{'} | |
| 3753 | f\left(x\right)=\left\{ \begin{array}{c} {\sin \left(\frac{\pi }{2}x\right)}x<-1 \\ \left|x\right|+kx\ge -1 \end{array}\right. | |
| 3754 | x=-1 | |
| 3755 | k=0 | |
| 3756 | k=1 | |
| 3757 | k=-1 | |
| 3758 | k=2 | |
| 3759 | k=-2 | |
| 3760 | f:\mathbb{R}\to \mathbb{R} | |
| 3761 | f | |
| 3762 | f^{'}\left(x_0\right)=f^{''}\left(x_0\right)=0 | |
| 3763 | x_0 | |
| 3764 | f\left(x\right)>0 | |
| 3765 | x | |
| 3766 | {\mathop{lim}_{x\to -\infty } f\left(x\right)}={\mathop{lim}_{x\to +\infty } f\left(x\right)}=0 | |
| 3767 | f | |
| 3768 | \mathbb{R} | |
| 3769 | f | |
| 3770 | x_0 | |
| 3771 | f | |
| 3772 | f^{''}\left(x_0\right)<0 | |
| 3773 | f | |
| 3774 | x_0 | |
| 3775 | f | |
| 3776 | f^{''}\left(x_0\right)>0 | |
| 3777 | f | |
| 3778 | f^{''}\left(x_0\right)<0 | |
| 3779 | x_0 | |
| 3780 | z | |
| 3781 | \left(z-\overline{z}\right)\overline{z}=2 | |
| 3782 | f\left(x\right)=x^2-3x+5 | |
| 3783 | g\left(x\right)=2x^2+3x-1 | |
| 3784 | 0 | |
| 3785 | 1 | |
| 3786 | 2 | |
| 3787 | 3 | |
| 3788 | f\left(x\right)=\frac{1}{x^2-3x+5} | |
| 3789 | g\left(x\right)=e^x | |
| 3790 | 0 | |
| 3791 | 1 | |
| 3792 | 2 | |
| 3793 | 3 | |
| 3794 | x{\cos \left(2x\right)}=500 | |
| 3795 | f\left(x\right)=\left|x^2-4x-5\right| | |
| 3796 | \left[-2,-4\right] | |
| 3797 | -1 | |
| 3798 | 2 | |
| 3799 | 2 | |
| 3800 | -1 | |
| 3801 | 5 | |
| 3802 | 2 | |
| 3803 | 7 | |
| 3804 | 27 | |
| 3805 | 9 | |
| 3806 | 0 | |
| 3807 | y=e^x{\ln \left(3-x\right)} | |
| 3808 | y=\frac{\sqrt{x}}{e^x} | |
| 3809 | x\ge 0 | |
| 3810 | \infty | |
| 3811 | x\to +\infty | |
| 3812 | \lim\limits_{x\to+\infty} f(x) = 4 | |
| 3813 | f(x) | |
| 3814 | \lim\limits_{x\to -\infty} f(x) = | |
| 3815 | - \infty | |
| 3816 | 0 | |
| 3817 | 4 | |
| 3818 | -4 | |
| 3819 | - \infty | |
| 3820 | f: A\to A | |
| 3821 | A | |
| 3822 | f^{-1}: A\to A | |
| 3823 | \lim\limits_{x \to a^-} f(x) = 2 | |
| 3824 | \lim\limits_{x\to a^+} f(x) = -\infty | |
| 3825 | f | |
| 3826 | x=a | |
| 3827 | f | |
| 3828 | x=a | |
| 3829 | y=f(a) | |
| 3830 | f | |
| 3831 | f | |
| 3832 | x=a | |
| 3833 | y=f(a) | |
| 3834 | f | |
| 3835 | \mathbb{R} | |
| 3836 | \mathbb{N} | |
| 3837 | \mathbb{N} | |
| 3838 | \mathbb{R} | |
| 3839 | f(x)=\sin(x)+\cos(x) | |
| 3840 | f(x)=\sin(x)-\cos(x) | |
| 3841 | f(x)=\tan(x) | |
| 3842 | f(x)=\cos(x)-\sin(x) | |
| 3843 | f(x)=1 | |
| 3844 | f(x)=2\sin(x) | |
| 3845 | f: \left[a, b\right]\to\mathbb{R} | |
| 3846 | f(x)=\ln(-x) | |
| 3847 | f(x) | |
| 3848 | f(x) | |
| 3849 | f(x) | |
| 3850 | f(x) | |
| 3851 | f(x)=\ln(3x^2) | |
| 3852 | f(x) | |
| 3853 | f(x) | |
| 3854 | f(x) | |
| 3855 | f(x) | |
| 3856 | f(x) | |
| 3857 | \ln(a\cdot b)=\ln(a)\cdot\ln(b) | |
| 3858 | \ln(a+b)=\ln(a)\cdot\ln(b) | |
| 3859 | \ln(\frac a b)=\frac{\left[\ln(a)+\ln(b)\right]}{2} | |
| 3860 | \ln(a\cdot b)=\ln(a)+\ln(b) | |
| 3861 | \ln(a-b)=\frac {\ln(a)}{\ln(b)} | |
| 3862 | f: \left[2, 3\right]\to\mathbb{R} | |
| 3863 | f(x)=6x^2 | |
| 3864 | f | |
| 3865 | 38 | |
| 3866 | 44 | |
| 3867 | 54 | |
| 3868 | f(x) | |
| 3869 | \frac {f^{'}(x)}{f(x)} | |
| 3870 | e^{f(x)}+c | |
| 3871 | \sin f(x)+c | |
| 3872 | \tan f(x)+c | |
| 3873 | \arcsin f(x)+c | |
| 3874 | \ln f(x) +c | |
| 3875 | f(x): \mathbb{R}\to\mathbb{R} | |
| 3876 | x=b | |
| 3877 | f(x) | |
| 3878 | x=b | |
| 3879 | f(x) | |
| 3880 | x=b | |
| 3881 | f(x) | |
| 3882 | x=b | |
| 3883 | f(x) | |
| 3884 | x=b | |
| 3885 | f(x)=\sin(2x)^2 | |
| 3886 | f(x) | |
| 3887 | 2\pi | |
| 3888 | f(x) | |
| 3889 | \pi | |
| 3890 | f(x) | |
| 3891 | x=0 | |
| 3892 | f(x) | |
| 3893 | x\to +\infty | |
| 3894 | f(x)=\frac{1-\cos x}{x} | |
| 3895 | \lim\limits_{x \to 0} f(x)^2=1 | |
| 3896 | \lim\limits_{x \to \pi} f(x)=\frac 1 2 | |
| 3897 | \lim\limits_{x \to 0} f(x)=\frac 1 2 | |
| 3898 | \lim\limits_{x \to \pi} f(x)=0 | |
| 3899 | \lim\limits_{x \to0} f(x)=0 | |
| 3900 | \frac{x+2}{\ln(x-4)} | |
| 3901 | x=0 | |
| 3902 | x=5 | |
| 3903 | x=5 | |
| 3904 | x=0 | |
| 3905 | x=5 | |
| 3906 | \mathbb{R} | |
| 3907 | \mathbb{R} | |
| 3908 | f(x)=e^{\left(x^2\right)} | |
| 3909 | f(x)=\sin\left(x^2\right) | |
| 3910 | f(x)=\ln\left[\left(x+2\right)^2\right] | |
| 3911 | f(x)=(x-3)^3 | |
| 3912 | f(x)=|x| | |
| 3913 | f(x)=x^2-3x | |
| 3914 | \left[2, 3\right] | |
| 3915 | x=3 | |
| 3916 | f(x)=e^{\ln\left[\left(x^2-9\right)^2\right]} | |
| 3917 | f(x)=\frac{2x-6}{x+3} | |
| 3918 | f(x)=\ln(x-2) | |
| 3919 | n | |
| 3920 | \mathbb{Q} | |
| 3921 | \mathbb{N} | |
| 3922 | \mathbb{R} | |
| 3923 | \mathbb{Q} | |
| 3924 | \mathbb{N} | |
| 3925 | f(x)=\sin\frac x 2 | |
| 3926 | x\to +\infty | |
| 3927 | 0 | |
| 3928 | 1 | |
| 3929 | 43132 | |
| 3930 | -1 | |
| 3931 | -0.5 | |
| 3932 | f: \left[a, b\right]\to\mathbb{R} | |
| 3933 | f | |
| 3934 | f | |
| 3935 | f | |
| 3936 | f | |
| 3937 | f\left(x\right)=\ln\left(x^2 \right)+\ln\left(x-3 \right) | |
| 3938 | \left(-\infty,+\infty\right) | |
| 3939 | \left(-\infty,3\right] | |
| 3940 | \left[3,+\infty\right) | |
| 3941 | \left(-\infty,3\right) | |
| 3942 | \left(3,+\infty\right) | |
| 3943 | f(x): I\to \mathbb{R} | |
| 3944 | f | |
| 3945 | f | |
| 3946 | f | |
| 3947 | f | |
| 3948 | \left(1,+\infty\right) | |
| 3949 | f(x)=\ln(x) | |
| 3950 | -1 | |
| 3951 | 1 | |
| 3952 | f(n)=\frac{1}{n^{\frac 1 2}} | |
| 3953 | f | |
| 3954 | \left[a, b\right]\to \mathbb{R} | |
| 3955 | \sup(f)=M | |
| 3956 | \inf(f)=-M | |
| 3957 | f | |
| 3958 | f | |
| 3959 | f | |
| 3960 | f | |
| 3961 | f: \left[a, b\right] \mapsto \mathbb{R} | |
| 3962 | f | |
| 3963 | \left[a, b\right] | |
| 3964 | f | |
| 3965 | \left(a, b\right) | |
| 3966 | f | |
| 3967 | \left[a, b\right] | |
| 3968 | f | |
| 3969 | \left[a, b\right] | |
| 3970 | f(n)=\frac {n!}{n^2} | |
| 3971 | \frac 1 2 | |
| 3972 | f(n)=\frac {(-1)^n}{n} | |
| 3973 | f(n) | |
| 3974 | n | |
| 3975 | 0 | |
| 3976 | n | |
| 3977 | f(n) | |
| 3978 | 0 | |
| 3979 | f(n) | |
| 3980 | 0 | |
| 3981 | f(x)=\ln(x) | |
| 3982 | f(x)=\sin(x) | |
| 3983 | f(x)=e^{x^2} | |
| 3984 | \left(n\to+\infty\right) | |
| 3985 | n | |
| 3986 | 0 | |
| 3987 | f(x)=a\cdot e^{2x} | |
| 3988 | f(x) | |
| 3989 | a | |
| 3990 | f^{'}(x) | |
| 3991 | a | |
| 3992 | f(x) | |
| 3993 | a | |
| 3994 | f^{'}(x) | |
| 3995 | a>0 | |
| 3996 | f(x) | |
| 3997 | f^{'}(x) | |
| 3998 | f^{'}(x) | |
| 3999 | \frac 1 {n^{\frac 1 3}} | |
| 4000 | 1 | |
| 4001 | 0 | |
| 4002 | f^{'}(x)>0 | |
| 4003 | f | |
| 4004 | f^{''}(x) | |
| 4005 | f(x)>f(x') | |
| 4006 | x>x' | |
| 4007 | f(x) | |
| 4008 | f(x)=\ln(x-1) | |
| 4009 | \ln(x) | |
| 4010 | z=4+i | |
| 4011 | 17 | |
| 4012 | 5 | |
| 4013 | \sqrt{5} | |
| 4014 | \sqrt{17} | |
| 4015 | z=3-5i | |
| 4016 | 34 | |
| 4017 | \sqrt{8} | |
| 4018 | \sqrt{34} | |
| 4019 | 2 | |
| 4020 | z=e^{2\pi i} | |
| 4021 | 2\pi | |
| 4022 | \sqrt{2\pi} | |
| 4023 | 1 | |
| 4024 | \sqrt{2} | |
| 4025 | z=e^{\frac \pi 3 i} | |
| 4026 | \frac {\sqrt{3}} 2 | |
| 4027 | \sqrt{3} | |
| 4028 | \pi | |
| 4029 | \frac \pi 3 | |
| 4030 | \frac 3 \pi | |
| 4031 | f(x)=x | |
| 4032 | \log(x) | |
| 4033 | \mathbb{R} | |
| 4034 | \lim\limits_{n\to\infty} \left(1+\frac 1 n\right)^n | |
| 4035 | \sqrt{3} | |
| 4036 | e | |
| 4037 | \infty | |
| 4038 | 0 | |
| 4039 | \lim\limits_{n\to\infty} \frac 1 n | |
| 4040 | \infty | |
| 4041 | 1 | |
| 4042 | 0 | |
| 4043 | f(x)=\log(x) | |
| 4044 | g(x)=x | |
| 4045 | x\to + \infty | |
| 4046 | f(x)\sim g(x) | |
| 4047 | f(x)=o(g(x)) | |
| 4048 | g(x)=o(f(x)) | |
| 4049 | f(x)=\sin(x) | |
| 4050 | g(x)=x | |
| 4051 | x\to+\infty | |
| 4052 | f(x)=o(g(x)) | |
| 4053 | f(x)\sim g(x) | |
| 4054 | g(x)=o(f(x)) | |
| 4055 | f(x)+g(x)=o(g(x)) | |
| 4056 | f(x)=\sin(x) | |
| 4057 | g(x)=x | |
| 4058 | x\to 0 | |
| 4059 | f(x)=o(g(x)) | |
| 4060 | g(x)=o(f(x)) | |
| 4061 | f(x)\sim g(x) | |
| 4062 | f(x)=\sqrt{x^2+x} | |
| 4063 | g(x)=x | |
| 4064 | x\to + \infty | |
| 4065 | f(x)=o(g(x)) | |
| 4066 | g(x)=o(f(x)) | |
| 4067 | f(x)-g(x)=0 | |
| 4068 | f(x)\sim g(x) | |
| 4069 | \frac {f(x)}{g(x)} \sim 4 | |
| 4070 | f | |
| 4071 | f | |
| 4072 | f | |
| 4073 | f | |
| 4074 | f | |
| 4075 | f | |
| 4076 | f | |
| 4077 | f | |
| 4078 | f | |
| 4079 | \left[a, b\right] | |
| 4080 | f(a)\cdot f(b)<0 | |
| 4081 | f | |
| 4082 | x_0 | |
| 4083 | f(x_0)=0 | |
| 4084 | f | |
| 4085 | \left[a, b\right] | |
| 4086 | f(a)\cdot f(b)<0 | |
| 4087 | \left[a, b\right] | |
| 4088 | f(a)=0 | |
| 4089 | f(b)=1 | |
| 4090 | 1 | |
| 4091 | \frac 1 2 | |
| 4092 | 0 | |
| 4093 | \left[a, b\right] | |
| 4094 | f(a)=f(b) | |
| 4095 | x_0 | |
| 4096 | f^{'}(x_0)=f(a) | |
| 4097 | f(x_0)=0 | |
| 4098 | f^{''}(x_0)=0 | |
| 4099 | f^{'}(x_0)=0 | |
| 4100 | f(x)=\log(x) | |
| 4101 | g(x)=x^3 | |
| 4102 | h(x)=3^x | |
| 4103 | x \to + \infty | |
| 4104 | g(x) |
| 4105 | h(x) |
| 4106 | f(x) |
| 4107 | g(x) |
| 4108 | f(x)=x^3 | |
| 4109 | h(x)=x! | |
| 4110 | g(x)=3^x | |
| 4111 | x\to + \infty | |
| 4112 | h(x) |
| 4113 | f(x) |
| 4114 | g(x) |
| 4115 | h(x) |
| 4116 | h(x)=x^x | |
| 4117 | g(x)=x! | |
| 4118 | f(x)=3^x | |
| 4119 | x\to + \infty | |
| 4120 | g(x) |
| 4121 | h(x) |
| 4122 | f(x) |
| 4123 | h(x) |
| 4124 | e^x | |
| 4125 | 1+x | |
| 4126 | 1-x | |
| 4127 | 1+x^2 | |
| 4128 | 1-x^2 | |
| 4129 | \sin(x) | |
| 4130 | 1+x | |
| 4131 | 1-x | |
| 4132 | x | |
| 4133 | x^2 | |
| 4134 | x^3 | |
| 4135 | \sin(x) | |
| 4136 | x | |
| 4137 | 1+x^2 | |
| 4138 | 1-x^2 | |
| 4139 | x+x^2 | |
| 4140 | x-x^2 | |
| 4141 | \cos(x) | |
| 4142 | 1+\frac{x^2}{2} | |
| 4143 | x^2 | |
| 4144 | 1-\frac{x^2}{2} | |
| 4145 | h=2+4i | |
| 4146 | z=3+\sqrt{11}i | |
| 4147 | |h|>|z| | |
| 4148 | |z|>|h| | |
| 4149 | |h|=|z| | |
| 4150 | |h|+|z|=0 | |
| 4151 | h=\sqrt{3}+2i | |
| 4152 | z=\sqrt{2}+5i | |
| 4153 | |z|>|h| | |
| 4154 | |z|<|h| | |
| 4155 | |z|=|h| | |
| 4156 | |z|+|h|=2 | |
| 4157 | z=e^{i\pi} | |
| 4158 | 1 | |
| 4159 | -1 | |
| 4160 | 0 | |
| 4161 | i | |
| 4162 | \pi | |
| 4163 | f | |
| 4164 | g | |
| 4165 | f+g | |
| 4166 | f+g | |
| 4167 | f+g | |
| 4168 | f | |
| 4169 | f | |
| 4170 | f | |
| 4171 | f^-1 | |
| 4172 | f(x)=x^2 | |
| 4173 | f | |
| 4174 | f | |
| 4175 | f | |
| 4176 | f(x)=x^3 | |
| 4177 | f(x)=\cos(x) | |
| 4178 | \cos(x) | |
| 4179 | \sin(x) | |
| 4180 | \tan(x) | |
| 4181 | \cos(x) | |
| 4182 | \sin(x) | |
| 4183 | x^2 | |
| 4184 | \ln(x) | |
| 4185 | \cos(x) | |
| 4186 | x^2 | |
| 4187 | f | |
| 4188 | f^-1 | |
| 4189 | \int_1^2 e^x \text{d}x | |
| 4190 | e^2 | |
| 4191 | e^2 -1 | |
| 4192 | e^2-e | |
| 4193 | e | |
| 4194 | \int_{1}^{2} e^x \text{d}x | |
| 4195 | e^2 | |
| 4196 | 2+e | |
| 4197 | e | |
| 4198 | e^2-e | |
| 4199 | f(x)=|x| | |
| 4200 | f | |
| 4201 | f | |
| 4202 | f | |
| 4203 | f | |
| 4204 | f(x)=|\log(x)| | |
| 4205 | f | |
| 4206 | f | |
| 4207 | f | |
| 4208 | f | |
| 4209 | f | |
| 4210 | g | |
| 4211 | \mathbb{R} | |
| 4212 | f+3g | |
| 4213 | \mathbb{R} | |
| 4214 | f\cdot g | |
| 4215 | \mathbb{R} | |
| 4216 | f | |
| 4217 | g | |
| 4218 | f-g | |
| 4219 | \mathbb{R} | |
| 4220 | f | |
| 4221 | g | |
| 4222 | \mathbb{R} | |
| 4223 | \frac f g | |
| 4224 | f\cdot g | |
| 4225 | f+g | |
| 4226 | f | |
| 4227 | g | |
| 4228 | \mathbb{R} | |
| 4229 | f+g | |
| 4230 | \frac f g | |
| 4231 | f+g | |
| 4232 | f | |
| 4233 | g | |
| 4234 | \mathbb{R} | |
| 4235 | f+g | |
| 4236 | f+g | |
| 4237 | f+g | |
| 4238 | f | |
| 4239 | -f | |
| 4240 | f | |
| 4241 | -f | |
| 4242 | \int_1^\infty \frac 1 {x^2} \text{d}x | |
| 4243 | \int_1^\infty \frac 1 x \text{d}x | |
| 4244 | \int_0^1 \frac 1 {x^2} \text{d}x | |
| 4245 | \int_1^\infty \frac {1}{\sqrt{x}} \text{d}x | |
| 4246 | \int_1^\infty \cos(x) \text{d}x | |
| 4247 | f(x)=e^x | |
| 4248 | g(x)=x | |
| 4249 | x\to \infty | |
| 4250 | f(x)=o(g(x)) | |
| 4251 | g(x)=o(f(x)) | |
| 4252 | g(x)\sim f(x) | |
| 4253 | f(x)=x^2 | |
| 4254 | g(x)=e^x | |
| 4255 | x\to \infty | |
| 4256 | f(x)=o(g(x)) | |
| 4257 | g(x)=o(f(x)) | |
| 4258 | g(x)\sim f(x) | |
| 4259 | f(x)=\log(x) | |
| 4260 | g(x)=x^x | |
| 4261 | x\to \infty | |
| 4262 | f(x)=o(g(x)) | |
| 4263 | g(x)=o(f(x)) | |
| 4264 | g(x)\sim f(x) | |
| 4265 | f(x)=\frac 1 {x^2} | |
| 4266 | g(x)=\frac 1 {x+x^2} | |
| 4267 | x\to \infty | |
| 4268 | f(x)=o(g(x)) | |
| 4269 | g(x)=o(f(x)) | |
| 4270 | g(x)\sim f(x) | |
| 4271 | f(x)=\sin(x) | |
| 4272 | g(x)=\cos(x) | |
| 4273 | x\to \infty | |
| 4274 | f(x)=o(g(x)) | |
| 4275 | g(x)=o(f(x)) | |
| 4276 | g(x)\sim f(x) | |
| 4277 | f(x)=\tan(x) | |
| 4278 | g(x)=\cos(x) | |
| 4279 | x\to \infty | |
| 4280 | f(x)=o(g(x)) | |
| 4281 | g(x)=o(f(x)) | |
| 4282 | g(x)\sim f(x) | |
| 4283 | f(x)=\sin(x) | |
| 4284 | g(x)=\tan(x) | |
| 4285 | x\to \infty | |
| 4286 | f(x)=o(g(x)) | |
| 4287 | g(x)=o(f(x)) | |
| 4288 | g(x)\sim f(x) | |
| 4289 | f(x)=3^x | |
| 4290 | g(x)=x^3 | |
| 4291 | x\to \infty | |
| 4292 | f(x)=o(g(x)) | |
| 4293 | g(x)=o(f(x)) | |
| 4294 | g(x)\sim f(x) | |
| 4295 | f(x)=10^x | |
| 4296 | g(x)=x^x | |
| 4297 | x\to \infty | |
| 4298 | f(x)=o(g(x)) | |
| 4299 | g(x)=o(f(x)) | |
| 4300 | g(x)\sim f(x) | |
| 4301 | f(x)=\sin(x) | |
| 4302 | g(x)=x | |
| 4303 | x\to 0 | |
| 4304 | f(x)=o(g(x)) | |
| 4305 | g(x)=o(f(x)) | |
| 4306 | g(x)\sim f(x) | |
| 4307 | f(x)=2-2\cos(x) | |
| 4308 | g(x)= x^2 | |
| 4309 | x\to 0 | |
| 4310 | f(x)=o(g(x)) | |
| 4311 | g(x)=o(f(x)) | |
| 4312 | g(x)\sim f(x) | |
| 4313 | f(x)=x | |
| 4314 | g(x)=x^3 | |
| 4315 | x\to 0 | |
| 4316 | f(x)=o(g(x)) | |
| 4317 | g(x)=o(f(x)) | |
| 4318 | g(x)\sim f(x) | |
| 4319 | f(x)=x | |
| 4320 | g(x)=\sqrt{x} | |
| 4321 | x\to 0 | |
| 4322 | f(x)=o(g(x)) | |
| 4323 | g(x)=o(f(x)) | |
| 4324 | g(x)\sim f(x) | |
| 4325 | f | |
| 4326 | x_0 | |
| 4327 | f^{'}(x_0)=0 | |
| 4328 | x_0 | |
| 4329 | f(x)=|x| | |
| 4330 | x_0=0 | |
| 4331 | f(x)=1/x | |
| 4332 | x_0=0 | |
| 4333 | f(x)=\sin(x) | |
| 4334 | \mathbb{R} | |
| 4335 | f(x)=\cos(x) | |
| 4336 | f(x)=\tan(x) | |
| 4337 | f(x)=e^x | |
| 4338 | f(x)=e^x | |
| 4339 | f(x)=x^2 | |
| 4340 | f(x)=\log(x) | |
| 4341 | f(x)=\arctan(x) | |
| 4342 | f(x)=\arccos(x) | |
| 4343 | f(x)=\arcsin(x) | |
| 4344 | f(x)=x^3 | |
| 4345 | I=\{x\in \mathbb{R}|x\geq 1\} | |
| 4346 | 0 | |
| 4347 | I=\{x\in \mathbb{R}|x>a\} | |
| 4348 | a | |
| 4349 | I | |
| 4350 | I | |
| 4351 | I | |
| 4352 | I | |
| 4353 | I=\{x\in \mathbb{R}|x\geq a\} | |
| 4354 | a | |
| 4355 | I | |
| 4356 | I | |
| 4357 | I | |
| 4358 | I | |
| 4359 | I=\{x\in \mathbb{R}|x\in \mathbb{Q}\} | |
| 4360 | I | |
| 4361 | e | |
| 4362 | \sqrt{2} | |
| 4363 | \pi | |
| 4364 | 3+2i | |
| 4365 | e^{\ln{\frac 3 2}} | |
| 4366 | 2^\pi | |
| 4367 | \sqrt{2} | |
| 4368 | (-2)^\pi | |
| 4369 | \pi | |
| 4370 | \pi^2 | |
| 4371 | \pi | |
| 4372 | 2^\pi | |
| 4373 | (-3)^{\sqrt{2}} | |
| 4374 | 0 | |
| 4375 | \sqrt{\pi} | |
| 4376 | z=3+2i | |
| 4377 | \bar{z} | |
| 4378 | 3+2i | |
| 4379 | 3-2i | |
| 4380 | 2+3i | |
| 4381 | 2i | |
| 4382 | 3 | |
| 4383 | z=5+2i | |
| 4384 | \bar{z} | |
| 4385 | 2+5i | |
| 4386 | 2-5i | |
| 4387 | 5+2i | |
| 4388 | 5-2i | |
| 4389 | 2 | |
| 4390 | z | |
| 4391 | j=e+ei | |
| 4392 | n | |
| 4393 | n | |
| 4394 | \mathbb{C} | |
| 4395 | \mathbb{R} | |
| 4396 | \mathbb{N} | |
| 4397 | \mathbb{Q} | |
| 4398 | n | |
| 4399 | \mathbb{R} | |
| 4400 | n | |
| 4401 | n | |
| 4402 | (n-1) | |
| 4403 | z_0 | |
| 4404 | -z_0 | |
| 4405 | z_0^2 | |
| 4406 | z_0^{-1} | |
| 4407 | \bar{z_0} | |
| 4408 | 0 | |
| 4409 | f | |
| 4410 | I(x_0) | |
| 4411 | x_0 | |
| 4412 | f(x_0)=0 | |
| 4413 | f(0)=0 | |
| 4414 | f^{'}(x_0)=0 | |
| 4415 | f^{''}(x_0)=0 | |
| 4416 | f | |
| 4417 | \left[a, b\right] | |
| 4418 | x_0 | |
| 4419 | f^{'}(x_0)=\frac {f(b)-f(a)}{b-a} | |
| 4420 | f^{'}(x_0)=0 | |
| 4421 | f(0)=\frac {f(b)-f(a)}{b-a} | |
| 4422 | f(1)=\frac {f(b)-f(a)}{b-a} | |
| 4423 | f(0)=\frac {f(x_0)-f(a)}{x_0-a} | |
| 4424 | \left[-1, 1\right] | |
| 4425 | x | |
| 4426 | \arcsin(x) | |
| 4427 | \arctan(x) | |
| 4428 | z^3 | |
| 4429 | \left[-1, 1\right] | |
| 4430 | x | |
| 4431 | x e^x | |
| 4432 | \log(x+100) | |
| 4433 | x^2 | |
| 4434 | \arctan(x) | |
| 4435 | \left[-1, 1\right] | |
| 4436 | \sin(x) | |
| 4437 | \cos(x) | |
| 4438 | x e^x | |
| 4439 | e^x | |
| 4440 | \tan(x) | |
| 4441 | \left[-1, 1\right] | |
| 4442 | |\tan(x)| | |
| 4443 | \cos(x) | |
| 4444 | x^2 | |
| 4445 | \left[-1, 1\right] | |
| 4446 | \cos(x) | |
| 4447 | x^2 | |
| 4448 | |\sin(x)| | |
| 4449 | \left[-1, 1\right] | |
| 4450 | \sqrt{x} | |
| 4451 | \log(x) | |
| 4452 | e^x | |
| 4453 | \left[-1, 1\right] | |
| 4454 | x^2 | |
| 4455 | \cos(x) | |
| 4456 | \arcsin(x) | |
| 4457 | \left[-1, 1\right] | |
| 4458 | \ln(x) | |
| 4459 | \frac 1 x | |
| 4460 | \sqrt{x} | |
| 4461 | \left[1, 2\right] | |
| 4462 | \log(x) | |
| 4463 | \sqrt{x} | |
| 4464 | \frac 1 x | |
| 4465 | f\left(x\right)=\cos\left(x\right) | |
| 4466 | \text{Im} \left(f\right) | |
| 4467 | (-1, 1) | |
| 4468 | [0, +\infty) | |
| 4469 | [0, 1] | |
| 4470 | [-1, 1] | |
| 4471 | (-\infty, 0] | |
| 4472 | f\left(x\right)=|\cos\left(x\right)| | |
| 4473 | \text{im} \left(f\right) | |
| 4474 | \left[0, 1\right] | |
| 4475 | \left[-1, 0\right] | |
| 4476 | \left[-1, 1\right] | |
| 4477 | \left(-1, 1\right) | |
| 4478 | \left(0, 1\right) | |
| 4479 | F = -kx | |
| 4480 | F = kx | |
| 4481 | F = kx^2 | |
| 4482 | F = \frac{k}{x} | |
| 4483 | F = \frac{x}{k} | |
| 4484 | \frac{kx^2}{2} | |
| 4485 | \frac{kx}{2} | |
| 4486 | kx | |
| 4487 | x^2k | |
| 4488 | \frac{x}{k^2} | |
| 4489 | I = VR^2 | |
| 4490 | V = \frac{R}{i} | |
| 4491 | V=Ri^2 | |
| 4492 | I=VR | |
| 4493 | V=Ri | |
| 4494 | F = \frac{KQq}{r^3} | |
| 4495 | F = \frac{KQq}{r^2} | |
| 4496 | F = \frac{KQq}{r} | |
| 4497 | F = \frac{Kq}{r^3} | |
| 4498 | F = \frac{Qq}{r^3} | |
| 4499 | U = \frac{KQq}{r^3} | |
| 4500 | U = \frac{KQq}{r^2} | |
| 4501 | U = \frac{KQq}{r} | |
| 4502 | U = \frac{KQ}{r^3} | |
| 4503 | U = \frac{Kq}{r^3} | |
| 4504 | P | |
| 4505 | P = R i^2 | |
| 4506 | P = \frac{V^2}{R} | |
| 4507 | P = Vi | |
| 4508 | t | |
| 4509 | W = Rit | |
| 4510 | W = Vi^2t | |
| 4511 | W = R\frac{i}{t} | |
| 4512 | W = Ri^2t | |
| 4513 | W = R\frac{i^2}{t} | |
| 4514 | O | |
| 4515 | P | |
| 4516 | \vec{M} = O\vec{P} \times \vec{F} | |
| 4517 | \vec{M} = \vec{F} \times O\vec{P} | |
| 4518 | \vec{M} = FO\vec{P} | |
| 4519 | \vec{M} = OP\vec{F} | |
| 4520 | \vec{M} = OPF | |
| 4521 | n | |
| 4522 | R | |
| 4523 | R_{eq} = \sum_{i} R_i | |
| 4524 | R_{eq} = \prod_{i} R_i | |
| 4525 | R_{eq} = \frac{1} {\sum_{i} R_i} | |
| 4526 | R_{eq} = \sum_{i} \frac{1}{R_i} | |
| 4527 | R_{eq} = \frac{1}{\prod_{i} R_i} | |
| 4528 | n | |
| 4529 | R | |
| 4530 | R_{eq} = \frac{1}{\sum_{i} R_i} | |
| 4531 | R_{eq} = \sum_{i} \frac{1}{R_i} | |
| 4532 | \frac{1}{R_{eq}} = \sum_{i} R_i | |
| 4533 | \frac{1}{R_{eq}} = \frac{1}{\sum_{i} R_i} | |
| 4534 | \frac{1}{R_{eq}} = \sum_{i} \frac{1}{R_i} | |
| 4535 | P | |
| 4536 | O | |
| 4537 | \vec{L} = O\vec{P} \times m\vec{v} | |
| 4538 | \vec{L} = O\vec{P} \times m\vec{a} | |
| 4539 | \vec{L} = OPm\vec{v} | |
| 4540 | \vec{L} = \vec{M} + m\vec{v} | |
| 4541 | \frac{d\vec{l}_0}{dt} | |
| 4542 | \vec{v}_0 \times m\vec{v}_{cm} | |
| 4543 | \vec{M}_e-\vec{v}_0 \times m\vec{v}_{cm} | |
| 4544 | \vec{M}_e | |
| 4545 | 0 | |
| 4546 | \vec{L}_0 | |
| 4547 | N | |
| 4548 | \vec{M}_0 | |
| 4549 | \vec{L}_0 | |
| 4550 | Nk | |
| 4551 | k | |
| 4552 | 3\cdot 10^{8} \frac{m}{s} | |
| 4553 | 2.9 \cdot 10^{23} \frac{m}{s} | |
| 4554 | 6\cdot 10^{2} \frac{m}{s} | |
| 4555 | 11\cdot 10^{-9} \frac{m}{s} | |
| 4556 | 1.8\cdot 10^{3} \frac{m}{s} | |
| 4557 | \frac{\lambda}{2m} | |
| 4558 | \frac{k}{m} | |
| 4559 | \frac{2\lambda dx}{dt} | |
| 4560 | \omega x | |
| 4561 | \frac{\lambda}{2 \omega} | |
| 4562 | \frac{\delta}{\omega} | |
| 4563 | \Sigma | |
| 4564 | E | |
| 4565 | \Sigma | |
| 4566 | E | |
| 4567 | \Sigma | |
| 4568 | E | |
| 4569 | \Sigma | |
| 4570 | \Sigma | |
| 4571 | D | |
| 4572 | \Sigma | |
| 4573 | \nabla j + \frac{d\sigma}{dt} = 0 | |
| 4574 | \nabla j = \frac{d\sigma}{dt} | |
| 4575 | \nabla j + \frac{d\sigma}{dt} = cost | |
| 4576 | \nabla j - \frac{d\sigma}{dt} = cost | |
| 4577 | \frac{d\sigma}{dt} = \frac{1}{\nabla j} | |
| 4578 | \vec{F}_e = \frac{d\vec{Q}}{dt} | |
| 4579 | \vec{F}_e = m\vec{Q} | |
| 4580 | \vec{F}_e = m\vec{V} | |
| 4581 | \vec{F}_e = m\vec{v}+\frac{d\vec{Q}}{dt} | |
| 4582 | \vec{F}_e = m\vec{v}+\frac{d\vec{L}}{dt} | |
| 4583 | \frac{d\vec{L_0}}{dt} = \vec{M}_0-\vec{v}_o \times m\vec{v}_{cm} | |
| 4584 | \frac{\vec{dL_0}}{dt} = \vec{M_0} | |
| 4585 | \frac{d\vec{L_0}}{dt} = \vec{M_0}+\vec{v_o} \times m\vec{v}_{cm} | |
| 4586 | \frac{\vec{dL_0}}{dt} =0 | |
| 4587 | \frac{\vec{dM_0}}{dt} =0 | |
| 4588 | I\omega | |
| 4589 | L\omega | |
| 4590 | M\omega | |
| 4591 | \frac{1}{2}I \omega^2 | |
| 4592 | \frac{1}{2}L \omega^2 | |
| 4593 | \alpha | |
| 4594 | I\omega \alpha | |
| 4595 | I\alpha | |
| 4596 | M\alpha | |
| 4597 | IM | |
| 4598 | I\omega | |
| 4599 | I\omega | |
| 4600 | M\alpha | |
| 4601 | I\alpha | |
| 4602 | MI | |
| 4603 | LI | |
| 4604 | \frac{1}{\sqrt{2}} | |
| 4605 | \sqrt{2} | |
| 4606 | \frac{1}{\sqrt{2}} | |
| 4607 | \sqrt{2} | |
| 4608 | \omega^2=\frac{g}{l} | |
| 4609 | \omega | |
| 4610 | \omega | |
| 4611 | \omega ^2 | |
| 4612 | \omega ^2 | |
| 4613 | \sqrt{\omega} | |
| 4614 | \alpha | |
| 4615 | \alpha | |
| 4616 | \alpha | |
| 4617 | \alpha | |
| 4618 | \alpha | |
| 4619 | \omega | |
| 4620 | \sqrt{\frac{g}{L}} | |
| 4621 | \sqrt{\frac{L}{g}} | |
| 4622 | \frac{g}{L} | |
| 4623 | \frac{L}{g} | |
| 4624 | \alpha | |
| 4625 | \alpha | |
| 4626 | \alpha | |
| 4627 | \alpha | |
| 4628 | \alpha | |
| 4629 | \rho | |
| 4630 | V | |
| 4631 | g | |
| 4632 | F=\frac{\rho g}{V} | |
| 4633 | F=\frac{gV}{\rho} | |
| 4634 | F=\rho gV | |
| 4635 | F=\frac{V}{\rho g} | |
| 4636 | F=\frac{g}{\rho V} | |
| 4637 | 273 \ K | |
| 4638 | 0 | |
| 4639 | 0 | |
| 4640 | 273 \ K | |
| 4641 | 0 | |
| 4642 | \frac{g}{3} | |
| 4643 | \frac{g}{9} | |
| 4644 | 3g | |
| 4645 | 9g | |
| 4646 | 6g | |
| 4647 | 45^\circ | |
| 4648 | M | |
| 4649 | E | |
| 4650 | E | |
| 4651 | D | |
| 4652 | B | |
| 4653 | \Sigma | |
| 4654 | \int{B \cdot \vec{u}_n d\Sigma} | |
| 4655 | \int {\frac{B \cdot \vec{u}_n} {d{\Sigma}}} | |
| 4656 | \int {B d\Sigma} | |
| 4657 | \int {\vec{u}_n d\Sigma} | |
| 4658 | \int {B \times \vec{u}_n d\Sigma} | |
| 4659 | q | |
| 4660 | m | |
| 4661 | v | |
| 4662 | B | |
| 4663 | q | |
| 4664 | m | |
| 4665 | v | |
| 4666 | B | |
| 4667 | F = q v B | |
| 4668 | F = q v B \sin \theta | |
| 4669 | F = \frac{q v B}{\sin \theta} | |
| 4670 | F = \frac{q v}{B} \sin \theta | |
| 4671 | F = \frac{q}{v} B \sin \theta | |
| 4672 | B | |
| 4673 | E | |
| 4674 | B | |
| 4675 | d\vec{F}=id\vec{s} \times \vec{B} | |
| 4676 | d\vec{F}=d\vec{s} \times \vec{B} | |
| 4677 | d\vec{F}=jd\vec{s} \times \vec{B} | |
| 4678 | d\vec{F}=id\vec{s} \vec{B} | |
| 4679 | d\vec{F}=i\frac{d\vec{s}} {\vec{B}} | |
| 4680 | l | |
| 4681 | B | |
| 4682 | F = l B \sin \theta | |
| 4683 | F = l B \cos \theta | |
| 4684 | F = i l B \sin \theta | |
| 4685 | F = i l B \cos \theta | |
| 4686 | F = i l B | |
| 4687 | F | |
| 4688 | S | |
| 4689 | F | |
| 4690 | S | |
| 4691 | F | |
| 4692 | S | |
| 4693 | F | |
| 4694 | S | |
| 4695 | F | |
| 4696 | S | |
| 4697 | 45^\circ | |
| 4698 | F | |
| 4699 | S | |
| 4700 | 135^\circ | |
| 4701 | 0 | |
| 4702 | 1 | |
| 4703 | 1 | |
| 4704 | C | |
| 4705 | i | |
| 4706 | \sigma | |
| 4707 | C | |
| 4708 | W=i \Delta \phi | |
| 4709 | W=-i \Delta \phi | |
| 4710 | W=\frac{i} {\Delta \phi} | |
| 4711 | W=-\frac{i} {\Delta \phi} | |
| 4712 | W=i^2 \Delta \phi | |
| 4713 | \frac{Kg}{A s^2} | |
| 4714 | \frac{Kg}{A s} | |
| 4715 | KgAs^2 | |
| 4716 | KgAs | |
| 4717 | \frac{KgA}{s^2} | |
| 4718 | \frac{kg}{A s^2} | |
| 4719 | \vec{B}=\frac{\mu_0i}{4\pi} \frac{\int(\vec{ds} \times \vec{u_r})}{r^2} | |
| 4720 | \vec{B}=\frac{\int(\vec{ds} \times \vec{u_r})}{r^2} | |
| 4721 | \vec{B}=\frac{\mu_0i}{4\pi} \int(\vec{ds} \times \vec{u_r})r^2 | |
| 4722 | \vec{B}= \frac{\int(\vec{ds} \times \vec{u_r})}{r^2} | |
| 4723 | \vec{B}=\frac{\mu_0i}{4\pi} \frac{\int(\vec{ds} \times \vec{u_r})}{r} | |
| 4724 | \vec{B} =\frac{\mu_0}{4\pi}\frac{q\vec{v} \times \vec{u_r}}{r^2} | |
| 4725 | B | |
| 4726 | \vec{B} =\frac{\mu_0}{4\pi}\frac{q\vec{v} \times \vec{u_r}}{r^2} | |
| 4727 | \vec{B} =\frac{\mu_0}{4\pi}q\vec{v} \times \vec{u_r}r^2 | |
| 4728 | \vec{B} =\frac{q\vec{v} \times \vec{u_r}}{r^2} | |
| 4729 | \vec{B}=q\vec{v} \times \vec{u_r} | |
| 4730 | \vec{B}=\frac{\mu_0}{4\pi} \frac{q \vec{v} \times \vec{u_r}}{r} | |
| 4731 | \nabla \times B=0 | |
| 4732 | \nabla B=0 | |
| 4733 | \nabla \times B=\mu_0 j | |
| 4734 | \nabla B=0 | |
| 4735 | \nabla \times B=0 | |
| 4736 | \nabla B=\mu_0 j | |
| 4737 | \nabla \times B=\frac{1}{\mu_0}j | |
| 4738 | \nabla B=0 | |
| 4739 | \nabla \times B=0 | |
| 4740 | \nabla B=\frac{1}{\mu_0}j | |
| 4741 | H | |
| 4742 | \nabla \times H = 0 | |
| 4743 | \nabla \times H = \mu_0 J | |
| 4744 | \nabla \times H = J | |
| 4745 | \nabla \times H = \mu_0 | |
| 4746 | \nabla \times H = \frac{1}{\mu_0} | |
| 4747 | H | |
| 4748 | H = \frac{B}{\mu_0} - M | |
| 4749 | H = B\mu_0 - M | |
| 4750 | H = \frac{B}{\mu_0} + M | |
| 4751 | H = B\mu_0 + M | |
| 4752 | H = B-M\mu_0 | |
| 4753 | H | |
| 4754 | M | |
| 4755 | m | |
| 4756 | \theta | |
| 4757 | 10 \ kg | |
| 4758 | 98\ N | |
| 4759 | 10\ N | |
| 4760 | 45\ N | |
| 4761 | 450\ N | |
| 4762 | 890\ N | |
| 4763 | 36 \ \frac{km}{h} | |
| 4764 | \frac{m}{s} | |
| 4765 | 0,36\ \frac{m}{s} | |
| 4766 | 36000\ \frac{m}{s} | |
| 4767 | 36\ \frac{m}{s} | |
| 4768 | 10 \ \frac{m}{s} | |
| 4769 | 100 \ \frac{m}{s} | |
| 4770 | r | |
| 4771 | v | |
| 4772 | mvr^2 | |
| 4773 | \frac{mv^2}{r} | |
| 4774 | \frac{1}{2} \frac{mv^2}{r} | |
| 4775 | \frac{vr^2}{m} | |
| 4776 | \frac{vm}{2} | |
| 4777 | 100 \ \frac{km}{h} | |
| 4778 | O | |
| 4779 | O | |
| 4780 | T | |
| 4781 | 1 | |
| 4782 | 25 \ \frac{J}{K mole} | |
| 4783 | 200 \ \frac{J}{K mole} | |
| 4784 | 151.6 \ \frac{J}{K mole} | |
| 4785 | 67.6 \ \frac{J}{K mole} | |
| 4786 | 273.15 \ \frac{J}{K mole} | |
| 4787 | T | |
| 4788 | 1 | |
| 4789 | 1 \ cal = 4186.8 \ J | |
| 4790 | 4 \ cal = 1.2 \ J | |
| 4791 | 1 \ cal = -4186 \ J | |
| 4792 | 1 \ cal = 0,412 \ J | |
| 4793 | 4 \ cal = 1486.6 \ J | |
| 4794 | dW=pdV | |
| 4795 | \gamma | |
| 4796 | 1 \ m | |
| 4797 | 2 \ cm^2 | |
| 4798 | 0,80 \ m | |
| 4799 | 0,1 \ m^2 | |
| 4800 | 1,40 \ m | |
| 4801 | 1 \ cm^2 | |
| 4802 | 2 \ m | |
| 4803 | 1 \ cm^2 | |
| 4804 | 0,1 \ m | |
| 4805 | 0,1 \ cm^2 | |
| 4806 | \Delta G < 0 | |
| 4807 | \Delta H > 0 | |
| 4808 | \Delta S = 0 | |
| 4809 | \Delta G > 0 | |
| 4810 | \Delta S < 0 | |
| 4811 | 10 \ m | |
| 4812 | 0,1 \ atm | |
| 4813 | 1 \ atm | |
| 4814 | 2 \ atm | |
| 4815 | 5 \ atm | |
| 4816 | 10 \ atm | |
| 4817 | 620-750 \ nm | |
| 4818 | 1 \ m | |
| 4819 | 1,5 \ m | |
| 4820 | 90 \ m | |
| 4821 | 40 \ m | |
| 4822 | 60 \ m | |
| 4823 | 80 \ m | |
| 4824 | 100 \ m | |
| 4825 | 135 \ m | |
| 4826 | 5 \ N | |
| 4827 | 10 \ N | |
| 4828 | 5 \ N | |
| 4829 | 25 \ N | |
| 4830 | 50 \ N | |
| 4831 | T^2 | |
| 4832 | a^3 | |
| 4833 | T^2 | |
| 4834 | a^3 | |
| 4835 | T^2 | |
| 4836 | a^3 | |
| 4837 | \vec{q}_{fin} - \vec{q}_{in} | |
| 4838 | \vec{L}_{fin} - \vec{L}_{in} | |
| 4839 | \vec{q}_{in} - \vec{q}_{fin} | |
| 4840 | \vec{L}_{in} - \vec{L}_{fin} | |
| 4841 | \vec{q}_{in} - \vec{q}_{fin} = \int_{t_{in}}^{t_{fin}} \vec{F} \,dt | |
| 4842 | \vec{q}_{fin} - \vec{q}_{in} = \int_{t_{in}}^{t_{fin}} \vec{F} \,dt | |
| 4843 | \vec{L}_{fin} - \vec{L}_{in} = \int_{t_{fin}}^{t_{in}} \vec{F} \,dt | |
| 4844 | \vec{L}_{fin} - \vec{L}_{in} = \int_{t_{in}}^{t_{fin}} \vec{L} \,dt | |
| 4845 | \vec{q}_{fin} - \vec{q}_{in} = \vec{L}_{fin} - \vec{L}_{in} | |
| 4846 | \vec{q}_{fin} - \vec{q}_{in} = \int_{t_{in}}^{t_{fin}} \vec{F} \,dt | |
| 4847 | \vec{q}_{in} - \vec{q}_{fin} = \int_{t_{in}}^{t_{fin}} \vec{M} \,dt | |
| 4848 | \vec{L}_{in} - \vec{L}_{fin} = \int_{t_{in}}^{t_{fin}} \vec{F} \,dt | |
| 4849 | \vec{L}_{fin} - \vec{L}_{in} = \int_{t_{in}}^{t_{fin}} \vec{M} \,dt | |
| 4850 | \vec{L}_{fin} - \vec{L}_{in} = 0 | |
| 4851 | \vec{q}_{fin} - \vec{q}_{in} = \int_{t_{in}}^{t_{fin}} \vec{F} \,dt | |
| 4852 | \vec{k}_{fin} - \vec{k}_{in} = \int_{t_{in}}^{t_{fin}} \vec{F} \,d\vec{r} | |
| 4853 | \vec{k}_{in} - \vec{k}_{fin} = \int_{x_{in}}^{x_{fin}} \vec{F} \,dt | |
| 4854 | \vec{k}_{fin} - \vec{k}_{in} = \int_{x_{fin}}^{x_{in}} \vec{F} \,dt | |
| 4855 | \vec{w} \times (\vec{a} \times \vec{r}) | |
| 4856 | \vec{w} \times (\vec{v} \times \vec{r}) | |
| 4857 | \vec{M} \times (\vec{w} \times \vec{r}) | |
| 4858 | \vec{w} \times (\vec{w} \times \vec{r}) | |
| 4859 | \vec{L} \times (\vec{w} \times \vec{r}) | |
| 4860 | \vec{w} \times \vec{w} \times \vec{v} | |
| 4861 | 2\vec{w} \times \vec{v} | |
| 4862 | \vec{w} \times \vec{v} | |
| 4863 | -\vec{w} \times (\vec{w} \times \vec{r}) | |
| 4864 | -m\vec{w} \times (\vec{w} \times \vec{r}) | |
| 4865 | -m \times (\vec{w} \times \vec{r}) | |
| 4866 | -m\vec{r} \times (\vec{w} \times \vec{r}) | |
| 4867 | -m\vec{w} \times (\vec{w} \times \vec{v}) | |
| 4868 | -m\vec{\omega} \times \vec v | |
| 4869 | -2m\vec{\omega} \times \vec r | |
| 4870 | -2m\vec{\omega} \times \vec v | |
| 4871 | -4m\vec{\omega} \times \vec v | |
| 4872 | -2m\vec{\omega}r \times \vec v | |
| 4873 | \pi GM | |
| 4874 | GM | |
| 4875 | 0 | |
| 4876 | \pi KG | |
| 4877 | QG\pi | |
| 4878 | 0 | |
| 4879 | KG\pi | |
| 4880 | UG\pi | |
| 4881 | MK | |
| 4882 | \vec Q = M\vec{a_{cm}} | |
| 4883 | \vec Q = \vec{L} \times \vec{a_{cm}} | |
| 4884 | \vec Q = MG | |
| 4885 | \vec Q = \vec{v} \times \vec{a_{cm}} | |
| 4886 | \vec Q = M\vec{v_{cm}} | |
| 4887 | Q \vec{a}_{cm} | |
| 4888 | M \vec{v}_{cm} | |
| 4889 | M \vec{a}_{cm} | |
| 4890 | M \vec{Q} | |
| 4891 | 0 | |
| 4892 | \vec{M}_o=\vec{R}_g \times M\vec{V}_g + \vec{l}_g | |
| 4893 | \vec{L}_o=\vec{R}_g \times M\vec{V}_g + \vec{l}_g | |
| 4894 | \vec{Q}_o=\vec{R}_g \times M\vec{V}_g + \vec{l}_g | |
| 4895 | \vec{L}_o=\vec{R}_g \times M\vec{A}_g + \vec{l}_g | |
| 4896 | \vec{L}_o=\vec{M}_o \times M\vec{V}_g + \vec{l}_g | |
| 4897 | K=\frac{1}{2}M{a_g}^2 + k_g | |
| 4898 | K=\frac{3}{2}M{V_g}^2 + k_g | |
| 4899 | K=M{V_g}^2 + k_g | |
| 4900 | K=\frac{1}{2}M{v_g}^2 + k_g | |
| 4901 | K=0 | |
| 4902 | \alpha | |
| 4903 | L_\alpha \omega_\alpha | |
| 4904 | I_\alpha \omega_\alpha | |
| 4905 | I_\alpha M_\alpha | |
| 4906 | M_\alpha \omega_\alpha | |
| 4907 | L_\alpha M_\alpha | |
| 4908 | L | |
| 4909 | L^2 | |
| 4910 | \frac{1}{12}ML^2 | |
| 4911 | \frac{1}{12}ML^3 | |
| 4912 | ML^2 | |
| 4913 | \frac{1}{2}w | |
| 4914 | \frac{1}{2}\vec{w} \times \vec{l_g} | |
| 4915 | \vec{w}\vec{l_g} | |
| 4916 | \frac{1}{2}\vec{w} \vec{l_g} | |
| 4917 | \frac{3}{2}\vec{w} \times \vec{l_g} | |
| 4918 | L | |
| 4919 | 0 | |
| 4920 | \frac{1}{12}ML^2 | |
| 4921 | \frac{1}{2}WLg | |
| 4922 | ML^2 | |
| 4923 | ML^3 | |
| 4924 | R | |
| 4925 | 0 | |
| 4926 | \frac{1}{2}MR^2 | |
| 4927 | MR^2 | |
| 4928 | \frac{M}{R} | |
| 4929 | \frac{M}{2R} | |
| 4930 | R | |
| 4931 | \frac{1}{2}MR^2 | |
| 4932 | \frac{1}{2}M^2 | |
| 4933 | MR^2 | |
| 4934 | \frac{1}{2}R^2 | |
| 4935 | R^2 | |
| 4936 | R | |
| 4937 | \frac{1}{2}R^2 | |
| 4938 | 0 | |
| 4939 | MR^2 | |
| 4940 | \frac{1}{2}MR^2 | |
| 4941 | R | |
| 4942 | \frac{1}{2}MR^2 | |
| 4943 | \frac{1}{3}MR^2 | |
| 4944 | \frac{1}{4}MR^2 | |
| 4945 | MR^2 | |
| 4946 | \frac{1}{4}R^2 | |
| 4947 | I | |
| 4948 | d | |
| 4949 | I+{d^2} | |
| 4950 | {I^2}+d | |
| 4951 | {I^2}+Md | |
| 4952 | {I+Md} | |
| 4953 | I+M{d^2} | |
| 4954 | \varepsilon | |
| 4955 | \varepsilon>1 | |
| 4956 | \varepsilon=1 | |
| 4957 | 0<\varepsilon<1 | |
| 4958 | \varepsilon=0 | |
| 4959 | \varepsilon | |
| 4960 | \varepsilon>1 | |
| 4961 | \varepsilon=1 | |
| 4962 | 0<\varepsilon<1 | |
| 4963 | \varepsilon=0 | |
| 4964 | \varepsilon | |
| 4965 | \varepsilon>1 | |
| 4966 | \varepsilon=1 | |
| 4967 | 0<\varepsilon<1 | |
| 4968 | \varepsilon=0 | |
| 4969 | \varepsilon | |
| 4970 | \varepsilon>1 | |
| 4971 | \varepsilon=1 | |
| 4972 | 0<\varepsilon<1 | |
| 4973 | \varepsilon=0 | |
| 4974 | 1\ km/h | |
| 4975 | 100\ km/h | |
| 4976 | km | |
| 4977 | 200\ km/h | |
| 4978 | 150\ km/h | |
| 4979 | 90 | |
| 4980 | 90 | |
| 4981 | 90 | |
| 4982 | y | |
| 4983 | x | |
| 4984 | x | |
| 4985 | h | |
| 4986 | h | |
| 4987 | h | |
| 4988 | h | |
| 4989 | q | |
| 4990 | \sigma | |
| 4991 | R | |
| 4992 | E | |
| 4993 | E | |
| 4994 | E | |
| 4995 | E | |
| 4996 | E | |
| 4997 | q | |
| 4998 | \sigma | |
| 4999 | R | |
| 5000 | E | |
| 5001 | E | |
| 5002 | E | |
| 5003 | E | |
| 5004 | E | |
| 5005 | E | |
| 5006 | 3\ \Omega | |
| 5007 | 2\ \Omega | |
| 5008 | 5\ \Omega | |
| 5009 | 10\ \Omega | |
| 5010 | 325\ \Omega | |
| 5011 | 532\ \Omega | |
| 5012 | 5003.002\ \Omega | |
| 5013 | 2003.005\ \Omega | |
| 5014 | d\Sigma | |
| 5015 | i | |
| 5016 | dm = id\Sigma \mu_n | |
| 5017 | i | |
| 5018 | h | |
| 5019 | \frac{D^2 x(t)}{dt^2} + \omega^2 x(t) = 0 | |
| 5020 | \frac{D^2 x(t)}{dt^2} - \omega^2 x(t) = 0 | |
| 5021 | \frac{D^2 x(t)}{dt^2} + \omega x(t) = 0 | |
| 5022 | \frac{D^2 x(t)}{dt^2} - \omega x(t) = 0 | |
| 5023 | \frac{D^2 x(t)}{dt^2}{\omega^2 x(t)} = 0 | |
| 5024 | f\colon\ [0,4]\to \mathbb{R} | |
| 5025 | \lim_{x \to 2}(f(x)) | |
| 5026 | f(2)=0 | |
| 5027 | f^{'}(x) | |
| 5028 | x=2 | |
| 5029 | f(x) | |
| 5030 | x=2 | |
| 5031 | f^{'}(x) | |
| 5032 | x | |
| 5033 | [0,4] | |
| 5034 | 0 | |
| 5035 | 0 | |
| 5036 | R=0 | |
| 5037 | M=0 | |
| 5038 | T=0 | |
| 5039 | \omega =0 | |
| 5040 | v=0 | |
| 5041 | v=0 | |
| 5042 | R=0 | |
| 5043 | v=0 | |
| 5044 | 0 | |
| 5045 | 1 | |
| 5046 | \infty | |
| 5047 | 2 | |
| 5048 | 3 | |
| 5049 | 4 | |
| 5050 | 3 | |
| 5051 | 4 | |
| 5052 | 5 | |
| 5053 | M | |
| 5054 | \sqrt{\frac{2M}{R}} | |
| 5055 | \frac{2GM}{R} | |
| 5056 | \sqrt{\frac{2GM}{R}} | |
| 5057 | \sqrt{\frac{2G}{R}} | |
| 5058 | \sqrt{\frac{GM}{R}} | |
| 5059 | \frac{N}{{Kg}^2} | |
| 5060 | \frac{N{m^2}}{{Kg}^2} | |
| 5061 | \frac{N{m^3}}{{Kg}^2} | |
| 5062 | \frac{m^2}{{Kg}^2} | |
| 5063 | Nm^2 | |
| 5064 | M | |
| 5065 | R | |
| 5066 | -\frac{GM}{R^2} | |
| 5067 | 0 | |
| 5068 | -\frac{M}{R^2} | |
| 5069 | -\frac{G}{R^2} | |
| 5070 | -\frac{GM}{R^3} | |
| 5071 | M | |
| 5072 | R | |
| 5073 | r | |
| 5074 | -\frac{G}{r^2} | |
| 5075 | -\frac{GM}{r^2} | |
| 5076 | 0 | |
| 5077 | -\frac{M}{r^2} | |
| 5078 | -\frac{GM}{r} | |
| 5079 | M | |
| 5080 | \pi GM | |
| 5081 | 4\pi GM | |
| 5082 | -\pi GM | |
| 5083 | -4\pi GM | |
| 5084 | -4\pi M | |
| 5085 | Q | |
| 5086 | 0 | |
| 5087 | 4\pi Q | |
| 5088 | 4\pi K | |
| 5089 | \pi KQ | |
| 5090 | 4\pi KQ | |
| 5091 | \mu | |
| 5092 | \frac{2\mu}{r} | |
| 5093 | \frac{k\mu}{r} | |
| 5094 | \frac{2k}{r} | |
| 5095 | \frac{2k\mu}{r} | |
| 5096 | 2k\mu | |
| 5097 | \sigma | |
| 5098 | \frac{\sigma}{2\epsilon_0} | |
| 5099 | \frac{\sigma}{\epsilon_0} | |
| 5100 | \sigma 2\epsilon_0 | |
| 5101 | \left(\frac{\sigma}{2\epsilon_0} \right)^2 | |
| 5102 | \frac{\sigma^2}{2\epsilon_0} | |
| 5103 | \sigma | |
| 5104 | \epsilon_0 | |
| 5105 | \frac{\sigma}{2\epsilon_0} | |
| 5106 | \frac{\sigma}{\epsilon_0} | |
| 5107 | -\sigma 2\epsilon_0 | |
| 5108 | \sigma 2\epsilon_0 | |
| 5109 | \sigma +2\epsilon_0 | |
| 5110 | \sigma | |
| 5111 | \epsilon_0 | |
| 5112 | d | |
| 5113 | -\sigma d\epsilon_0 | |
| 5114 | -\frac{\sigma d}{\epsilon_0} | |
| 5115 | \frac{\sigma d}{\epsilon_0} | |
| 5116 | -\frac{\sigma}{\epsilon_0} | |
| 5117 | \rho | |
| 5118 | p+\rho gz = cost. | |
| 5119 | p+gz = cost. | |
| 5120 | p\rho z = cost. | |
| 5121 | p+gz = cost. | |
| 5122 | p+ \rho z = cost. | |
| 5123 | 1\ bar | |
| 5124 | 780\ mmHg | |
| 5125 | 1,071\ atm | |
| 5126 | 760\ mmHg | |
| 5127 | 760\ Pa | |
| 5128 | \frac{1}{2} \rho {v^2}+\rho g+p=cost. | |
| 5129 | \frac{1}{2} \rho {v^2}+\rho z+p=cost. | |
| 5130 | \frac{1}{2}\rho v+\rho gz+p=cost. | |
| 5131 | \frac{1}{2}\rho {v^2}+ \rho gz+p=cost. | |
| 5132 | \rho{v^2}+\rho gz+p=cost. | |
| 5133 | p=nRT | |
| 5134 | pV=nR | |
| 5135 | pV=nRT | |
| 5136 | pV=nT | |
| 5137 | pV=RT | |
| 5138 | 0\ K | |
| 5139 | +273.15^\circ C | |
| 5140 | 0^\circ C | |
| 5141 | -273.15^\circ C | |
| 5142 | 273,15\ Pa | |
| 5143 | -273,15\ Pa | |
| 5144 | {6,022}\cdot 10^{23} | |
| 5145 | {5,022}\cdot 10^{23} | |
| 5146 | {6,022}\cdot 10^{23} | |
| 5147 | {6,022}\cdot 10^{-23} | |
| 5148 | {K_b}T | |
| 5149 | \frac{3}{2} {T} | |
| 5150 | \frac{3}{2} {K_b} | |
| 5151 | \frac{3}{2} {K_b}{T} | |
| 5152 | \frac{3}{2} \frac{K_b}{T} | |
| 5153 | \frac{f}{2} \frac{K_b}{T} | |
| 5154 | \frac{f}{2} {K_b}T | |
| 5155 | \frac{3}{2} {K_b}T | |
| 5156 | \frac{f}{2} {K_b} | |
| 5157 | \frac{3}{2} {K_b}{T^2} | |
| 5158 | pV=K_bT | |
| 5159 | pV=NK_bT | |
| 5160 | pV=NK_b | |
| 5161 | pV=nRT | |
| 5162 | pV=NT | |
| 5163 | Q>0 | |
| 5164 | L>0 | |
| 5165 | dU=Q+L | |
| 5166 | dU=Q-L | |
| 5167 | dU=QL | |
| 5168 | dU=\frac{Q}{L} | |
| 5169 | dU=Q^L | |
| 5170 | U | |
| 5171 | 90 | |
| 5172 | 90 | |
| 5173 | 90 | |
| 5174 | 0 | |
| 5175 | 90 | |
| 5176 | 90 | |
| 5177 | 90 | |
| 5178 | 0 | |
| 5179 | m | |
| 5180 | r | |
| 5181 | 1 | |
| 5182 | 0 | |
| 5183 | 2\pi rm | |
| 5184 | 2\pi rwm | |
| 5185 | 2 \pi{r^2}{w^2} | |
| 5186 | 2\pi{r^2}{w^2}m | |
| 5187 | 0 | |
| 5188 | 0 | |
| 5189 | 0 | |
| 5190 | 0 | |
| 5191 | 0 | |
| 5192 | T | |
| 5193 | 2l | |
| 5194 | 4l | |
| 5195 | \frac{1}{2}l | |
| 5196 | \frac{1}{4}l | |
| 5197 | 10 \ kg | |
| 5198 | 10 \ kg | |
| 5199 | 10\ kg | |
| 5200 | 10 \ kg | |
| 5201 | 0 \ kg | |
| 5202 | v | |
| 5203 | \frac{N}{s} | |
| 5204 | \frac{Nm}{s} | |
| 5205 | \frac{Nm}{s^2} | |
| 5206 | \frac{Kgm}{s} | |
| 5207 | J | |
| 5208 | 1 kg | |
| 5209 | 28 kg \frac m s | |
| 5210 | 0 \frac m/s | |
| 5211 | 28 \frac m/s | |
| 5212 | 7.8 \frac m/s | |
| 5213 | 3.6 \frac m/s | |
| 5214 | T_1=800\ K | |
| 5215 | T_2=200\ K | |
| 5216 | 8\ kJ | |
| 5217 | 1\ kJ | |
| 5218 | 2\ kJ | |
| 5219 | 3\ kJ | |
| 5220 | 6\ kJ | |
| 5221 | 8\ kJ | |
| 5222 | 0 | |
| 5223 | 0 | |
| 5224 | 0 | |
| 5225 | 180 | |
| 5226 | 270 | |
| 5227 | T_A | |
| 5228 | T_B | |
| 5229 | T_A |
| 5230 | T_A=T_B | |
| 5231 | T_A>T_B | |
| 5232 | dT | |
| 5233 | \frac f 2 K_b \ dT | |
| 5234 | \frac f 2 \ dT | |
| 5235 | \frac f 2 R \ dT | |
| 5236 | \frac 1 2 K_b \ dT | |
| 5237 | \frac 3 2 K_b \ dT | |
| 5238 | dT | |
| 5239 | \frac f 2\ dT | |
| 5240 | \frac 1 2 K_b \ dT | |
| 5241 | \frac 3 2 K_b \ dT | |
| 5242 | \frac 1 2 R\ dT | |
| 5243 | \frac f 2 K_b \ dT | |
| 5244 | c_v\ dT | |
| 5245 | nc_p\ dT | |
| 5246 | nc_v\ dT | |
| 5247 | nc_v | |
| 5248 | nc_p | |
| 5249 | nc_v\ d | |
| 5250 | c_v\ dT | |
| 5251 | nc_p | |
| 5252 | nc_v\ dT | |
| 5253 | nc_p\ dT | |
| 5254 | c_p=\frac {c_v}{R} | |
| 5255 | c_p=c_v R | |
| 5256 | c_p=R | |
| 5257 | c_p=c_v-R | |
| 5258 | c_p=c_v+R | |
| 5259 | c_p | |
| 5260 | \frac 3 2 R | |
| 5261 | \frac 5 2 R | |
| 5262 | \frac 7 2 R | |
| 5263 | \frac 9 2 R | |
| 5264 | \frac 11 2 R | |
| 5265 | c_v | |
| 5266 | \frac 1 2 R | |
| 5267 | \frac 3 2 R | |
| 5268 | \frac 5 2 R | |
| 5269 | \frac 7 2 R | |
| 5270 | \frac 9 2 R | |
| 5271 | \frac {L_{syst}}{Q_{ced}} | |
| 5272 | \frac {L_{syst}}{Q_{ass}} | |
| 5273 | \frac {L_{syst}}{Q_{tot}} | |
| 5274 | \frac {L_{amb}}{Q_{ced}} | |
| 5275 | \frac {L_{amb}}{Q_{ass}} | |
| 5276 | nc_v\ dT | |
| 5277 | c_v dT | |
| 5278 | nc_p | |
| 5279 | nc_v | |
| 5280 | nc_p\ dT | |
| 5281 | Q | |
| 5282 | nR\ln\left(\frac{T_f}{T_i}\right) | |
| 5283 | nc_v\ dT | |
| 5284 | L | |
| 5285 | \frac f 2 K_b\ dT | |
| 5286 | nc_p | |
| 5287 | nc_v | |
| 5288 | nRT | |
| 5289 | 0 | |
| 5290 | nc_v\ dT | |
| 5291 | nc_p\ dT | |
| 5292 | 0 | |
| 5293 | nRT\ln\left(\frac{V_f}{V_i}\right) | |
| 5294 | \frac 1 3 rm^2 | |
| 5295 | \frac 3 8 mr^3 | |
| 5296 | \frac 1 2 m^2 r^2 | |
| 5297 | \frac 2 5 mr^2 | |
| 5298 | \frac 1 3 mr^2 | |
| 5299 | N | |
| 5300 | Kg \frac m s | |
| 5301 | \frac N s | |
| 5302 | N \frac m s | |
| 5303 | N | |
| 5304 | Kg\frac m s | |
| 5305 | \frac N s | |
| 5306 | N \frac m s | |
| 5307 | N\frac m s | |
| 5308 | \frac N s | |
| 5309 | J | |
| 5310 | \frac J s | |
| 5311 | 1 | |
| 5312 | 2 | |
| 5313 | 3 | |
| 5314 | 4 | |
| 5315 | 5 | |
| 5316 | G | |
| 5317 | 8 | |
| 5318 | 4 | |
| 5319 | 6 | |
| 5320 | 2 | |
| 5321 | 1 | |
| 5322 | 10^5\ Pa | |
| 5323 | 10^4\ Pa | |
| 5324 | 10^5\ mmHg | |
| 5325 | 10^5\ atm | |
| 5326 | 2\ kNm^2 | |
| 5327 | 10^3\ Pa | |
| 5328 | 1\ MNm^2 | |
| 5329 | 10^7\ Pa | |
| 5330 | 10^5\ Pa | |
| 5331 | 0 | |
| 5332 | 0^{\circ} | |
| 5333 | 45^{\circ} | |
| 5334 | 90^{\circ} | |
| 5335 | 145^{\circ} | |
| 5336 | 270^{\circ} | |
| 5337 | N\cdot m\cdot s | |
| 5338 | N\cdot \frac m s | |
| 5339 | kg\cdot m\cdot s | |
| 5340 | kg\cdot \frac m s | |
| 5341 | N\cdot m | |
| 5342 | N\cdot m\cdot s | |
| 5343 | N\cdot \frac m s | |
| 5344 | N\cdot m | |
| 5345 | kg\cdot m\cdot s | |
| 5346 | kg\cdot \frac m s | |
| 5347 | J | |
| 5348 | kg\cdot m | |
| 5349 | kg\cdot \frac m s | |
| 5350 | kg\cdot m\cdot s | |
| 5351 | N\cdot m\cdot s | |
| 5352 | N\cdot m | |
| 5353 | \frac{N}{m} | |
| 5354 | N | |
| 5355 | N\cdot m^2 | |
| 5356 | 0 | |
| 5357 | 0 | |
| 5358 | 1 | |
| 5359 | 1 | |
| 5360 | 1 | |
| 5361 | 0 | |
| 5362 | 1 | |
| 5363 | 1 | |
| 5364 | 1 | |
| 5365 | 1 | |
| 5366 | \frac R L | |
| 5367 | R\cdot L | |
| 5368 | \frac L R | |
| 5369 | R+L | |
| 5370 | \frac N C | |
| 5371 | \frac V C | |
| 5372 | \frac A V | |
| 5373 | \frac C V | |
| 5374 | \frac C m | |
| 5375 | \frac{J}{Kg\cdot K} | |
| 5376 | \frac{J}{K} | |
| 5377 | J\cdot K | |
| 5378 | \frac{J}{mol\cdot K} | |
| 5379 | \frac{J}{K^2} | |
| 5380 | 1 | |
| 5381 | 1 | |
| 5382 | 0 | |
| 5383 | 1 | |
| 5384 | 0 | |
| 5385 | 90 | |
| 5386 | 0 | |
| 5387 | 180 | |
| 5388 | L | |
| 5389 | i | |
| 5390 | B | |
| 5391 | F=\frac {iB} L | |
| 5392 | F=\frac {BL} i | |
| 5393 | F=\frac {Li} B | |
| 5394 | F=\frac B {iL} | |
| 5395 | F=iBL | |
| 5396 | \frac {cal\cdot g} K | |
| 5397 | \frac K {cal\cdot g} | |
| 5398 | \frac g {cal\cdot K} | |
| 5399 | \frac cal {g\cdot K} | |
| 5400 | \frac {cal\cdot K} g | |
| 5401 | \frac {g} {cal\cdot K} | |
| 5402 | \frac {cal} {g} | |
| 5403 | \frac {g} {cal} | |
| 5404 | \frac {cal\cdot g} {K} | |
| 5405 | \frac {cal} {g\cdot K} | |
| 5406 | 1 \ ^{\circ} C | |
| 5407 | 1\ g | |
| 5408 | 14,5\ ^{\circ} C | |
| 5409 | 1,5 \ J | |
| 5410 | 10 \ erg | |
| 5411 | 5 \ kcal | |
| 5412 | 2,5 \ kWh | |
| 5413 | 1 \ cal | |
| 5414 | 0 | |
| 5415 | 10\ \Omega | |
| 5416 | 20\ V | |
| 5417 | 5 \ A | |
| 5418 | 10 \ A | |
| 5419 | 2 \ A | |
| 5420 | 20 \ A | |
| 5421 | 200 \ A | |
| 5422 | J | |
| 5423 | K | |
| 5424 | \frac{K}{J} | |
| 5425 | \frac{K}{mol} | |
| 5426 | \frac{J}{K} | |
| 5427 | 3 | |
| 5428 | \frac 1 9 | |
| 5429 | 6 | |
| 5430 | 9 | |
| 5431 | \frac 1 3 | |
| 5432 | 5F | |
| 5433 | 30F | |
| 5434 | 30 | |
| 5435 | 5 | |
| 5436 | 25 | |
| 5437 | 6 | |
| 5438 | 43252 | |
| 5439 | 100\ ^{\circ} C | |
| 5440 | -273\ ^{\circ} C | |
| 5441 | 0\ ^{\circ} C | |
| 5442 | -40\ ^{\circ} C | |
| 5443 | 57\ ^{\circ} C | |
| 5444 | 0 | |
| 5445 | 1 | |
| 5446 | 0 | |
| 5447 | 1 | |
| 5448 | P=IV | |
| 5449 | P=\frac I V | |
| 5450 | P=\frac V I | |
| 5451 | P=\frac 1 {IV} | |
| 5452 | x | |
| 5453 | k | |
| 5454 | F=\frac k x | |
| 5455 | F=-kx | |
| 5456 | F=\frac x k | |
| 5457 | F=-\frac x k | |
| 5458 | F=kx | |
| 5459 | 8 | |
| 5460 | 4 | |
| 5461 | 2\ kg | |
| 5462 | 20\ m | |
| 5463 | 10\ \frac m s | |
| 5464 | 20\ \frac m s | |
| 5465 | 30\ \frac m s | |
| 5466 | 60\ \frac m s | |
| 5467 | 80\ \frac m s | |
| 5468 | 2\ kg | |
| 5469 | 20\ m | |
| 5470 | 5\ J | |
| 5471 | 100\ J | |
| 5472 | 200\ J | |
| 5473 | 400\ J | |
| 5474 | 800\ J | |
| 5475 | 100\ \frac N m | |
| 5476 | 2\ m | |
| 5477 | 200\ J | |
| 5478 | 25\ J | |
| 5479 | 50\ J | |
| 5480 | 400\ J | |
| 5481 | 100\ J | |
| 5482 | \frac 1 4 | |
| 5483 | 200\ \frac N m | |
| 5484 | 50\ N | |
| 5485 | 0,05\ m | |
| 5486 | 0,10\ m | |
| 5487 | 0,15\ m | |
| 5488 | 0,20\ m | |
| 5489 | 0,25\ m | |
| 5490 | |a+b| \leq |a|+|b| | |
| 5491 | |a+b| \geq |a|-|b| | |
| 5492 | |a+b| \leq |b|-|a| | |
| 5493 | |a| \geq a | |
| 5494 | |a+b+c| \leq |a|+|b+c| | |
| 5495 | \mathbb{N} \subset \mathbb{R} \subset \mathbb{Q} | |
| 5496 | \mathbb{Q} \subset \mathbb{R} \subset \mathbb{N} | |
| 5497 | \mathbb{R} \subset \mathbb{Q} \subset \mathbb{N} | |
| 5498 | \mathbb{R} \subset \mathbb{N} \subset \mathbb{Q} | |
| 5499 | \mathbb{N} \subset \mathbb{Q} \subset \mathbb{R} | |
| 5500 | W | |
| 5501 | \frac{J}{s} | |
| 5502 | CV | |
| 5503 | eV | |
| 5504 | \frac{cal}{s} | |
| 5505 | \frac 1 2 | |
| 5506 | \frac 1 2 | |
| 5507 | \frac 1 2 | |
| 5508 | \frac 1 2 | |
| 5509 | 0,01 \ m | |
| 5510 | 50 \ \frac V m | |
| 5511 | 0,5\ V | |
| 5512 | 5\ V | |
| 5513 | 50\ V | |
| 5514 | 100\ V | |
| 5515 | 0,05\ V | |
| 5516 | 1 F | |
| 5517 | 2 F | |
| 5518 | 3 F | |
| 5519 | 1,5 F | |
| 5520 | \frac 2 3 F | |
| 5521 | 2,5 F | |
| 5522 | 1 F | |
| 5523 | U | |
| 5524 | x | |
| 5525 | 2U | |
| 5526 | \frac U 2 | |
| 5527 | 4U | |
| 5528 | \frac U 4 | |
| 5529 | \left[ \sqrt{2} , \pi \right) | |
| 5530 | V\cdot R | |
| 5531 | \frac V L | |
| 5532 | \frac L R | |
| 5533 | \frac V R | |
| 5534 | R\cdot L | |
| 5535 | \frac R C | |
| 5536 | \frac C V | |
| 5537 | \frac V {RC} | |
| 5538 | \frac C R | |
| 5539 | C\cdot V | |
| 5540 | \frac V R | |
| 5541 | R \cdot C | |
| 5542 | \frac C V | |
| 5543 | \frac R C | |
| 5544 | C\cdot V | |
| 5545 | 10 | |
| 5546 | -3 | |
| 5547 | -6 | |
| 5548 | -9 | |
| 5549 | -12 | |
| 5550 | -15 | |
| 5551 | 0^{\circ} | |
| 5552 | 45^{\circ} | |
| 5553 | 90^{\circ} | |
| 5554 | 135^{\circ} | |
| 5555 | 180^{\circ} | |
| 5556 | \frac L T | |
| 5557 | \frac 1 T | |
| 5558 | T | |
| 5559 | \frac 1 L | |
| 5560 | \frac T L | |
| 5561 | X | |
| 5562 | A | |
| 5563 | I\left(x\right) | |
| 5564 | x | |
| 5565 | A | |
| 5566 | x | |
| 5567 | A | |
| 5568 | x | |
| 5569 | A | |
| 5570 | x | |
| 5571 | A | |
| 5572 | P\cdot T | |
| 5573 | \frac P T | |
| 5574 | P\cdot V | |
| 5575 | \frac V T | |
| 5576 | \frac P V | |
| 5577 | V\Delta P | |
| 5578 | 0 | |
| 5579 | V\Delta T | |
| 5580 | P\Delta T | |
| 5581 | P\Delta V | |
| 5582 | R\Delta T | |
| 5583 | R\Delta V | |
| 5584 | T\Delta P | |
| 5585 | P\Delta T | |
| 5586 | Cv | |
| 5587 | Cp | |
| 5588 | R | |
| 5589 | R=\frac Cv Cp | |
| 5590 | R=Cp-Cv | |
| 5591 | R=Cp\cdot Cv | |
| 5592 | R=Cv-Cp | |
| 5593 | R=Cp+Cv | |
| 5594 | \frac {Kg} {m^3} | |
| 5595 | \frac {Kg} {m^2} | |
| 5596 | \frac {Kg} m | |
| 5597 | N\cdot m^2 | |
| 5598 | \frac Kg m | |
| 5599 | \frac m N | |
| 5600 | kg\cdot m^2 | |
| 5601 | N | |
| 5602 | 2 \ kg | |
| 5603 | 5 \ m | |
| 5604 | 50\ kg\cdot m^2 | |
| 5605 | 25\ kg\cdot m^2 | |
| 5606 | \frac {100} {3} \ kg\cdot m^2 | |
| 5607 | 20\ kg\cdot m^2 | |
| 5608 | \frac {10} {3} \ kg\cdot m^2 | |
| 5609 | 5\ \Omega | |
| 5610 | 200\ V | |
| 5611 | 20 A | |
| 5612 | 1000 A | |
| 5613 | 100 A | |
| 5614 | 40 A | |
| 5615 | 400 A | |
| 5616 | V | |
| 5617 | N | |
| 5618 | Pa | |
| 5619 | C | |
| 5620 | A | |
| 5621 | di risorse e posizioni? | |
| 5622 | sanzione?? | |
| 5623 | reali saranno le conseguenze"? | |
| 5624 | \frac{C}{N\cdot m} | |
| 5625 | \frac{N}{m\cdot C} | |
| 5626 | \frac{C}{m^2} | |
| 5627 | \frac{F}{m} | |
| 5628 | A | |
| 5629 | V | |
| 5630 | \frac{J}{C} | |
| 5631 | \frac{N\cdot m}{C} | |
| 5632 | ad una situazione? | |
| 5633 | 10^13 | |
| 5634 | 10^9 | |
| 5635 | 10^15 | |
| 5636 | 10^12 | |
| 5637 | G_1 | |
| 5638 | G_2 | |
| 5639 | G_1 | |
| 5640 | G_2 | |
| 5641 | G_1 | |
| 5642 | G_2 | |
| 5643 | G_1 | |
| 5644 | G_2 | |
| 5645 | G_1 | |
| 5646 | G_2 | |
| 5647 | H^+ | |
| 5648 | OH^– | |
| 5649 | H^– | |
| 5650 | OH^+ | |
| 5651 | OH^– | |
| 5652 | n^2(n | |
| 5653 | H^+ | |
| 5654 | H^+ | |
| 5655 | OH^– | |
| 5656 | OH^– | |
| 5657 | H_2 | |
| 5658 | cm^3 | |
| 5659 | dm^3 | |
| 5660 | H^+ | |
| 5661 | OH^– | |
| 5662 | H^+ | |
| 5663 | OH^– | |
| 5664 | H_2S | |
| 5665 | H_2SO_4 | |
| 5666 | H_2SO_3 | |
| 5667 | Na_2SO_4 | |
| 5668 | K_2S | |
| 5669 | 10^–27 | |
| 5670 | 10^–27 | |
| 5671 | 10^–17 | |
| 5672 | 10^–35 | |
| 5673 | 10^–27 | |
| 5674 | Cl_2O_3 | |
| 5675 | NH_3 | |
| 5676 | Al_2O_3 | |
| 5677 | Na_2O | |
| 5678 | Ca_3(PO_4)_2 | |
| 5679 | CaPO_4 | |
| 5680 | Ca_3(PO_4)_3 | |
| 5681 | Ca_3(HPO_4)_2 | |
| 5682 | Ca_3P_2 | |
| 5683 | Mg(OH)_2 | |
| 5684 | MgH_2 | |
| 5685 | O_2 | |
| 5686 | H_2O_2 | |
| 5687 | OH^– | |
| 5688 | H_2MgO | |
| 5689 | 1/2O_2 | |
| 5690 | 2NaNO_3 | |
| 5691 | 2NaNO_2 | |
| 5692 | O_2 | |
| 5693 | 3NaNO_2 | |
| 5694 | O_2 | |
| 5695 | 2NaNO_3 | |
| 5696 | 2NaNO_2 | |
| 5697 | 3/2O_2 | |
| 5698 | NaNO_3 | |
| 5699 | NaNO_2 | |
| 5700 | O_2 | |
| 5701 | 2NaNO_3 | |
| 5702 | 2NaNO_2 | |
| 5703 | 3O_2 | |
| 5704 | SO_3 | |
| 5705 | SO_2 | |
| 5706 | SO_4 | |
| 5707 | H_2S | |
| 5708 | H_2SO_4 | |
| 5709 | KH(IO_3)_2 | |
| 5710 | KHIO_3 | |
| 5711 | KHI_2 | |
| 5712 | KH(IO)_2 | |
| 5713 | H_3PO_4 | |
| 5714 | H_2PO_3 | |
| 5715 | H_2PO_4 | |
| 5716 | H_3PO_3 | |
| 5717 | H_4PO_4 | |
| 5718 | Ba(HSO_4)_2 | |
| 5719 | Ba(HSO_3)_2 | |
| 5720 | BaSO_4 | |
| 5721 | Ba(HS)_2 | |
| 5722 | BaH_2SO_4 | |
| 5723 | HCO_3^– | |
| 5724 | (CO_3^2–)_2 | |
| 5725 | H_2CO_3^– | |
| 5726 | CO_2^2– | |
| 5727 | Na_2S | |
| 5728 | Na_2SO_3 | |
| 5729 | NaSO_4 | |
| 5730 | Na_2SO_4 | |
| 5731 | CO_3^2– | |
| 5732 | CO_2^– | |
| 5733 | HCO_3^– | |
| 5734 | CO_3^2+ | |
| 5735 | HCO_2^– | |
| 5736 | HClO_4 | |
| 5737 | HClO_3 | |
| 5738 | HClO_2 | |
| 5739 | Nb_2O_5 | |
| 5740 | NbO_3 | |
| 5741 | Nb_2O_3 | |
| 5742 | Nb_2O_4 | |
| 5743 | Nb_4O_10 | |
| 5744 | NaH_2PO_4 | |
| 5745 | H_5PO_3 | |
| 5746 | KCl_2 | |
| 5747 | H_3CO_3 | |
| 5748 | CaH_2SO_3 | |
| 5749 | Ca_3(PO_4)_2 | |
| 5750 | Ca_3(PO_3)_2 | |
| 5751 | CaHPO_3 | |
| 5752 | CaHPO_4 | |
| 5753 | Ca_2(PO_4)_3 | |
| 5754 | MgO_2 | |
| 5755 | Mg(OH)_2 | |
| 5756 | Mg_2O_3 | |
| 5757 | ClO_4^– | |
| 5758 | Cl^– | |
| 5759 | ClO^– | |
| 5760 | ClO_2 | |
| 5761 | CO_2 | |
| 5762 | C_2O | |
| 5763 | C_2O_2 | |
| 5764 | C_2SO_2 | |
| 5765 | H_2S_2O_3 | |
| 5766 | H_2SO_4 | |
| 5767 | H_2SO_3 | |
| 5768 | H_2S | |
| 5769 | SO_2 | |
| 5770 | S_2O_3 | |
| 5771 | SO_3 | |
| 5772 | H_2SO_4 | |
| 5773 | Al(OH)_3 | |
| 5774 | Al_2O_3 | |
| 5775 | Al_3(OH)_3 | |
| 5776 | Al_2O | |
| 5777 | ^oC) | |
| 5778 | ^oC) | |
| 5779 | CO_3^2– | |
| 5780 | CO_2 | |
| 5781 | CO^2– | |
| 5782 | C^+ | |
| 5783 | Fe(OH)_3 | |
| 5784 | Fe(OH)_2 | |
| 5785 | Fe_2O_3 | |
| 5786 | FeH_2 | |
| 5787 | NaHCO_3 | |
| 5788 | Na_2CO_3 | |
| 5789 | CH_3COONa | |
| 5790 | CH_3COONH_4 | |
| 5791 | K_2SO_4 | |
| 5792 | H_2SO_5 | |
| 5793 | H_2SO_4 | |
| 5794 | H_2SO_3 | |
| 5795 | H_2S | |
| 5796 | H_2S_2O_7 | |
| 5797 | sp^2 | |
| 5798 | CH_3-CH_2-CH_3 | |
| 5799 | CH_4 | |
| 5800 | CH_3-CH_2-CH_2-CH_2-CH_3 | |
| 5801 | CH_3-CH_2-CH_2-CH_3 | |
| 5802 | sp^3 | |
| 5803 | sp^3 | |
| 5804 | sp^2 | |
| 5805 | sp^2 | |
| 5806 | sp^2 | |
| 5807 | sp^3 | |
| 5808 | sp^3 | |
| 5809 | sp^2 | |
| 5810 | CO_2 | |
| 5811 | H_2O | |
| 5812 | H_2O | |
| 5813 | CH_2Cl_2 | |
| 5814 | CH_2 | |
| 5815 | CCl_4 | |
| 5816 | CHCl_3 | |
| 5817 | CH_3-CH_2-COOH | |
| 5818 | CH_3-CH_2-CO-O-CO-CH_2-CH_3 | |
| 5819 | CH_3-CH_2-CHO | |
| 5820 | CH_3-CO-CH_3 | |
| 5821 | CH_3Cl | |
| 5822 | CH_3CH_2OH | |
| 5823 | C_6H_5Cl | |
| 5824 | CH_3COCl | |
| 5825 | CH_3OCH_3 | |
| 5826 | C_6H_6 | |
| 5827 | C_6H_14 | |
| 5828 | C_6H_12 | |
| 5829 | C_6H_10 | |
| 5830 | C_6H_8 | |
| 5831 | -NO_2 | |
| 5832 | -NH_2 | |
| 5833 | CH_4 | |
| 5834 | C_6H_6 | |
| 5835 | C_2H_6 | |
| 5836 | C_2H_4 | |
| 5837 | C_2H_5OH | |
| 5838 | CH_3OH | |
| 5839 | CH_3OCH_3 | |
| 5840 | CH_3NH_2 | |
| 5841 | NO_2 | |
| 5842 | NH_3 | |
| 5843 | CH_3CONH_2 | |
| 5844 | CH_3COOCH_3 | |
| 5845 | CH_3NO_2 | |
| 5846 | CH_3NHCH_3 | |
| 5847 | CH_3NH_2 | |
| 5848 | –NH_2 | |
| 5849 | RCONH_2 | |
| 5850 | CO_2 | |
| 5851 | H_2O | |
| 5852 | CO_2 | |
| 5853 | CO_2 | |
| 5854 | O_2 | |
| 5855 | H_2O | |
| 5856 | O_2 | |
| 5857 | CO_2 | |
| 5858 | H_2 | |
| 5859 | dell'O_2 | |
| 5860 | (l_0) | |
| 5861 | l_0 | |
| 5862 | l_0 | |
| 5863 | dell'O_2 | |
| 5864 | dell'HO_2 | |
| 5865 | CO_2 | |
| 5866 | dell'O_2 | |
| 5867 | H_2O | |
| 5868 | CO_2 | |
| 5869 | CO_2 | |
| 5870 | O_2 | |
| 5871 | CO_2 | |
| 5872 | H_2O | |
| 5873 | g/cm^3 | |
| 5874 | g/cm^3 | |
| 5875 | g/cm^3 | |
| 5876 | mg/cm^3 | |
| 5877 | mg/cm^3 | |
| 5878 | cm^3 | |
| 5879 | 10^–4 | |
| 5880 | cm^3 | |
| 5881 | 10^3 | |
| 5882 | cm^3 | |
| 5883 | cm^3 | |
| 5884 | cm^3 | |
| 5885 | w_C | |
| 5886 | w_T | |
| 5887 | w_C | |
| 5888 | w_T | |
| 5889 | w_C | |
| 5890 | w_T | |
| 5891 | w_C | |
| 5892 | 1/w_T | |
| 5893 | w_C | |
| 5894 | w_T | |
| 5895 | kg/m^3 | |
| 5896 | g/m^3 | |
| 5897 | g/m^3 | |
| 5898 | g/m^3 | |
| 5899 | kg/m^3 | |
| 5900 | m/s^2, | |
| 5901 | m/s^2, | |
| 5902 | m/s^2, | |
| 5903 | m/s^2, | |
| 5904 | m/s^2 | |
| 5905 | m/s^2 | |
| 5906 | m/s^2 | |
| 5907 | m/s^2 | |
| 5908 | m/s^2 | |
| 5909 | m/s^2 | |
| 5910 | m/s^2 | |
| 5911 | 3mv^2 | |
| 5912 | mv^2 | |
| 5913 | 2mv^2 | |
| 5914 | mv^2 | |
| 5915 | 5mv^2 | |
| 5916 | R_1 | |
| 5917 | R_2 | |
| 5918 | P_C > P_L | |
| 5919 | P_C < P_L | |
| 5920 | P_C = P_L | |
| 5921 | 9,81 \cdot P_C = P_L | |
| 5922 | V \cdot P_C = P_L | |
| 5923 | m^3 | |
| 5924 | m^3 | |
| 5925 | P_0 | |
| 5926 | P_0 | |
| 5927 | P_0/2 | |
| 5928 | m/s^2 | |
| 5929 | m/s^2 | |
| 5930 | m/s^2 | |
| 5931 | m/s^2 | |
| 5932 | m/s^2 | |
| 5933 | m/s^2 | |
| 5934 | m/s^2 | |
| 5935 | m/s^2 | |
| 5936 | m/s^2 | |
| 5937 | m/s^2 | |
| 5938 | d_fluido | |
| 5939 | N/m^3 | |
| 5940 | N/m^3 | |
| 5941 | N/m^2 | |
| 5942 | s^–1 | |
| 5943 | s^–1 | |
| 5944 | v = 4ms^{-1} | |
| 5945 | a = 2ms^{-2} | |
| 5946 | V_0 | |
| 5947 | V_0/2 | |
| 5948 | V_0/4 | |
| 5949 | 2V_0 | |
| 5950 | 4V_0 | |
| 5951 | 10^2 | |
| 5952 | µ_o· | |
| 5953 | µ_r· | |
| 5954 | m/s^2 | |
| 5955 | m/s^2 | |
| 5956 | m/s^2 | |
| 5957 | m/s^2 | |
| 5958 | m/s^2 | |
| 5959 | m/s^2 | |
| 5960 | m/s^2 | |
| 5961 | m/s^2 | |
| 5962 | m/s^2 | |
| 5963 | m/s^2 | |
| 5964 | m/s^2 | |
| 5965 | m/s^2 | |
| 5966 | m/s^2 | |
| 5967 | m/s^2 | |
| 5968 | m/s^2 | |
| 5969 | m^2 | |
| 5970 | m^2 | |
| 5971 | m^2 | |
| 5972 | m^2 | |
| 5973 | m^2 | |
| 5974 | km^2 | |
| 5975 | km^2 | |
| 5976 | km^2 | |
| 5977 | km^2 | |
| 5978 | km^2 | |
| 5979 | N_2 | |
| 5980 | O_3 | |
| 5981 | (m^3/s) | |
| 5982 | (m^3/anno) | |
| 5983 | sen^2(x) | |
| 5984 | cos^2(x) | |
| 5985 | cos^2(x) | |
| 5986 | sen^2(x) | |
| 5987 | sen^2(x) | |
| 5988 | cos^2(x) | |
| 5989 | cos^2 | |
| 5990 | sen^2 | |
| 5991 | cosα)^2 | |
| 5992 | cos^2α | |
| 5993 | sen^2α | |
| 5994 | cos^2α | |
| 5995 | sen^2α | |
| 5996 | \frac{1}{\sqrt{2}} | |
| 5997 | cos^2(x) | |
| 5998 | sen^2(x) | |
| 5999 | cos^2(x)) | |
| 6000 | cos^2(x) | |
| 6001 | sen^2(x) | |
| 6002 | sen^2(x) | |
| 6003 | cos^2(x) | |
| 6004 | sen^2(x)) | |
| 6005 | 2cos^2(x) | |
| 6006 | cot^2(x) | |
| 6007 | 1/cos^2(x) | |
| 6008 | cos^2(x) | |
| 6009 | sen^2(x) | |
| 6010 | cos^2(x)) | |
| 6011 | 2cos^3(α) | |
| 6012 | 3cos^2(α) | |
| 6013 | –2cos^3(α) | |
| 6014 | 3cos^2(α) | |
| 6015 | –cos^2(α) | |
| 6016 | 2cos^3(α) | |
| 6017 | cos^2(α) | |
| 6018 | cos^2(α) | |
| 6019 | 4sen(α)cos^2(α/2) | |
| 6020 | 4sen(α)cos^2(α) | |
| 6021 | 2sen^3(α) | |
| 6022 | –4sen^3(α) | |
| 6023 | –2sen^2(α) | |
| | | | | | | | | | | | | | | | | |